Index: docs/HB5_Expt/ATLAS_1808.00336/obs.dat =================================================================== --- docs/HB5_Expt/ATLAS_1808.00336/obs.dat (revision 0) +++ docs/HB5_Expt/ATLAS_1808.00336/obs.dat (revision 587) @@ -0,0 +1,14 @@ +260.0 0.10691264740207959 +274.9641226353555 0.15469851400310033 +300.06523157208085 0.20169079656674344 +324.6836268754077 0.14477252770831708 +350.2674494455316 0.0718173167629018 +399.9869536855838 0.039166523845135456 +450.18917155903455 0.029199286434471425 +500.3913894324853 0.026061585659671142 +549.6281800391389 0.007463033793611057 +599.8303979125897 0.009019886631186398 +699.7521200260926 0.010010555966512963 +800.1565557729941 0.009638313845927303 +900.0782778864971 0.005833699253497624 +999.5172863666014 0.009916168878524714 Index: docs/HB5_Expt/ATLAS_1808.00336/exp_interpol.dat =================================================================== --- docs/HB5_Expt/ATLAS_1808.00336/exp_interpol.dat (revision 0) +++ docs/HB5_Expt/ATLAS_1808.00336/exp_interpol.dat (revision 587) @@ -0,0 +1,149 @@ + 260.00 0.1869700 + 265.00 0.1938150 + 270.00 0.2006601 + 275.00 0.2075052 + 280.00 0.2003420 + 285.00 0.1931788 + 290.00 0.1860157 + 295.00 0.1788525 + 300.00 0.1716893 + 305.00 0.1599846 + 310.00 0.1482799 + 315.00 0.1365751 + 320.00 0.1248704 + 325.00 0.1131657 + 330.00 0.1092592 + 335.00 0.1053526 + 340.00 0.1014461 + 345.00 0.9753957E-01 + 350.00 0.9363304E-01 + 355.00 0.8874187E-01 + 360.00 0.8385070E-01 + 365.00 0.7895953E-01 + 370.00 0.7406837E-01 + 375.00 0.6917720E-01 + 380.00 0.6428603E-01 + 385.00 0.5939486E-01 + 390.00 0.5450370E-01 + 395.00 0.4961253E-01 + 400.00 0.4472136E-01 + 405.00 0.4268816E-01 + 410.00 0.4065496E-01 + 415.00 0.3862177E-01 + 420.00 0.3658857E-01 + 425.00 0.3455537E-01 + 430.00 0.3252217E-01 + 435.00 0.3048898E-01 + 440.00 0.2845578E-01 + 445.00 0.2642258E-01 + 450.00 0.2438939E-01 + 455.00 0.2368460E-01 + 460.00 0.2297981E-01 + 465.00 0.2227502E-01 + 470.00 0.2157023E-01 + 475.00 0.2086544E-01 + 480.00 0.2016065E-01 + 485.00 0.1945587E-01 + 490.00 0.1875108E-01 + 495.00 0.1804629E-01 + 500.00 0.1734150E-01 + 505.00 0.1687592E-01 + 510.00 0.1641034E-01 + 515.00 0.1594477E-01 + 520.00 0.1547919E-01 + 525.00 0.1501361E-01 + 530.00 0.1454803E-01 + 535.00 0.1408246E-01 + 540.00 0.1361688E-01 + 545.00 0.1315130E-01 + 550.00 0.1268572E-01 + 555.00 0.1259314E-01 + 560.00 0.1250055E-01 + 565.00 0.1240796E-01 + 570.00 0.1231537E-01 + 575.00 0.1222278E-01 + 580.00 0.1213019E-01 + 585.00 0.1203760E-01 + 590.00 0.1194501E-01 + 595.00 0.1185242E-01 + 600.00 0.1175983E-01 + 605.00 0.1163583E-01 + 610.00 0.1151184E-01 + 615.00 0.1138784E-01 + 620.00 0.1126385E-01 + 625.00 0.1113985E-01 + 630.00 0.1101585E-01 + 635.00 0.1089186E-01 + 640.00 0.1076786E-01 + 645.00 0.1064387E-01 + 650.00 0.1051987E-01 + 655.00 0.1039588E-01 + 660.00 0.1027188E-01 + 665.00 0.1014788E-01 + 670.00 0.1002389E-01 + 675.00 0.9899892E-02 + 680.00 0.9775897E-02 + 685.00 0.9651901E-02 + 690.00 0.9527905E-02 + 695.00 0.9403909E-02 + 700.00 0.9279914E-02 + 705.00 0.9218449E-02 + 710.00 0.9156985E-02 + 715.00 0.9095520E-02 + 720.00 0.9034056E-02 + 725.00 0.8972592E-02 + 730.00 0.8911127E-02 + 735.00 0.8849663E-02 + 740.00 0.8788199E-02 + 745.00 0.8726734E-02 + 750.00 0.8665270E-02 + 755.00 0.8603806E-02 + 760.00 0.8542341E-02 + 765.00 0.8480877E-02 + 770.00 0.8419413E-02 + 775.00 0.8357948E-02 + 780.00 0.8296484E-02 + 785.00 0.8235020E-02 + 790.00 0.8173555E-02 + 795.00 0.8112091E-02 + 800.00 0.8050626E-02 + 805.00 0.8024799E-02 + 810.00 0.7998971E-02 + 815.00 0.7973143E-02 + 820.00 0.7947315E-02 + 825.00 0.7921488E-02 + 830.00 0.7895660E-02 + 835.00 0.7869832E-02 + 840.00 0.7844004E-02 + 845.00 0.7818176E-02 + 850.00 0.7792349E-02 + 855.00 0.7766521E-02 + 860.00 0.7740693E-02 + 865.00 0.7714865E-02 + 870.00 0.7689037E-02 + 875.00 0.7663210E-02 + 880.00 0.7637382E-02 + 885.00 0.7611554E-02 + 890.00 0.7585726E-02 + 895.00 0.7559898E-02 + 900.00 0.7534071E-02 + 905.00 0.7537656E-02 + 910.00 0.7541242E-02 + 915.00 0.7544828E-02 + 920.00 0.7548413E-02 + 925.00 0.7551999E-02 + 930.00 0.7555585E-02 + 935.00 0.7559170E-02 + 940.00 0.7562756E-02 + 945.00 0.7566342E-02 + 950.00 0.7569927E-02 + 955.00 0.7573513E-02 + 960.00 0.7577099E-02 + 965.00 0.7580684E-02 + 970.00 0.7584270E-02 + 975.00 0.7587856E-02 + 980.00 0.7591441E-02 + 985.00 0.7595027E-02 + 990.00 0.7598612E-02 + 995.00 0.7602198E-02 + 1000.00 0.7605784E-02 Index: docs/HB5_Expt/ATLAS_1808.00336/data.dat =================================================================== --- docs/HB5_Expt/ATLAS_1808.00336/data.dat (revision 0) +++ docs/HB5_Expt/ATLAS_1808.00336/data.dat (revision 587) @@ -0,0 +1,154 @@ +# ATLAS, arXiv:1808.00336, August 2018, Fig. 2(top) +# 336_Atlas_X-HH-bbtautau_13TeV_36.1fb-1.txt +# limit set on sigma(pp->X)xBR(X->HH)xBR(H->tautau)xBR(H->bb) x 2 (in pb) +# MX obs exp + + 260.0 0.1069 0.1870 + 265.0 0.1228 0.1938 + 270.0 0.1388 0.2007 + 275.0 0.1547 0.2075 + 280.0 0.1641 0.2003 + 285.0 0.1735 0.1932 + 290.0 0.1829 0.1860 + 295.0 0.1923 0.1789 + 300.0 0.2017 0.1717 + 305.0 0.1903 0.1600 + 310.0 0.1789 0.1483 + 315.0 0.1675 0.1366 + 320.0 0.1562 0.1249 + 325.0 0.1448 0.1132 + 330.0 0.1302 0.1093 + 335.0 0.1156 0.1054 + 340.0 0.1010 0.1014 + 345.0 0.8641E-01 0.9754E-01 + 350.0 0.7182E-01 0.9363E-01 + 355.0 0.6855E-01 0.8874E-01 + 360.0 0.6529E-01 0.8385E-01 + 365.0 0.6202E-01 0.7896E-01 + 370.0 0.5876E-01 0.7407E-01 + 375.0 0.5549E-01 0.6918E-01 + 380.0 0.5223E-01 0.6429E-01 + 385.0 0.4896E-01 0.5939E-01 + 390.0 0.4570E-01 0.5450E-01 + 395.0 0.4243E-01 0.4961E-01 + 400.0 0.3917E-01 0.4472E-01 + 405.0 0.3817E-01 0.4269E-01 + 410.0 0.3717E-01 0.4065E-01 + 415.0 0.3618E-01 0.3862E-01 + 420.0 0.3518E-01 0.3659E-01 + 425.0 0.3418E-01 0.3456E-01 + 430.0 0.3319E-01 0.3252E-01 + 435.0 0.3219E-01 0.3049E-01 + 440.0 0.3119E-01 0.2846E-01 + 445.0 0.3020E-01 0.2642E-01 + 450.0 0.2920E-01 0.2439E-01 + 455.0 0.2889E-01 0.2368E-01 + 460.0 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+ 795.0 0.9657E-02 0.8112E-02 + 800.0 0.9638E-02 0.8051E-02 + 805.0 0.9448E-02 0.8025E-02 + 810.0 0.9258E-02 0.7999E-02 + 815.0 0.9068E-02 0.7973E-02 + 820.0 0.8877E-02 0.7947E-02 + 825.0 0.8687E-02 0.7921E-02 + 830.0 0.8497E-02 0.7896E-02 + 835.0 0.8307E-02 0.7870E-02 + 840.0 0.8116E-02 0.7844E-02 + 845.0 0.7926E-02 0.7818E-02 + 850.0 0.7736E-02 0.7792E-02 + 855.0 0.7546E-02 0.7767E-02 + 860.0 0.7356E-02 0.7741E-02 + 865.0 0.7165E-02 0.7715E-02 + 870.0 0.6975E-02 0.7689E-02 + 875.0 0.6785E-02 0.7663E-02 + 880.0 0.6595E-02 0.7637E-02 + 885.0 0.6404E-02 0.7612E-02 + 890.0 0.6214E-02 0.7586E-02 + 895.0 0.6024E-02 0.7560E-02 + 900.0 0.5834E-02 0.7534E-02 + 905.0 0.6038E-02 0.7538E-02 + 910.0 0.6242E-02 0.7541E-02 + 915.0 0.6446E-02 0.7545E-02 + 920.0 0.6650E-02 0.7548E-02 + 925.0 0.6854E-02 0.7552E-02 + 930.0 0.7058E-02 0.7556E-02 + 935.0 0.7263E-02 0.7559E-02 + 940.0 0.7467E-02 0.7563E-02 + 945.0 0.7671E-02 0.7566E-02 + 950.0 0.7875E-02 0.7570E-02 + 955.0 0.8079E-02 0.7574E-02 + 960.0 0.8283E-02 0.7577E-02 + 965.0 0.8487E-02 0.7581E-02 + 970.0 0.8691E-02 0.7584E-02 + 975.0 0.8896E-02 0.7588E-02 + 980.0 0.9100E-02 0.7591E-02 + 985.0 0.9304E-02 0.7595E-02 + 990.0 0.9508E-02 0.7599E-02 + 995.0 0.9712E-02 0.7602E-02 + 1000. 0.9916E-02 0.7606E-02 Index: docs/HB5_Expt/ATLAS_1808.00336/exp.dat =================================================================== --- docs/HB5_Expt/ATLAS_1808.00336/exp.dat (revision 0) +++ docs/HB5_Expt/ATLAS_1808.00336/exp.dat (revision 587) @@ -0,0 +1,14 @@ +260.0 0.18696995041286119 +274.9641226353555 0.20750517486469974 +300.06523157208085 0.17168931225920886 +325.16634050880623 0.11316569242148997 +350.2674494455316 0.09363303790303715 +399.9869536855838 0.0447213595499958 +450.18917155903455 0.024389385097531087 +500.3913894324853 0.017341499331979503 +550.1108936725375 0.01268572482532661 +600.3131115459882 0.011759829312576624 +700.2348336594912 0.009279913533608991 +800.6392694063927 0.008050626463312142 +900.5609915198957 0.007534070706754234 +1000.0 0.007605783785002441 Index: docs/HB5_Expt/ATLAS_1808.00336/obs_interpol.dat =================================================================== --- docs/HB5_Expt/ATLAS_1808.00336/obs_interpol.dat (revision 0) +++ docs/HB5_Expt/ATLAS_1808.00336/obs_interpol.dat (revision 587) @@ -0,0 +1,149 @@ + 260.00 0.1069126 + 265.00 0.1228413 + 270.00 0.1387699 + 275.00 0.1546985 + 280.00 0.1640970 + 285.00 0.1734954 + 290.00 0.1828939 + 295.00 0.1922923 + 300.00 0.2016908 + 305.00 0.1903071 + 310.00 0.1789235 + 315.00 0.1675398 + 320.00 0.1561562 + 325.00 0.1447725 + 330.00 0.1301815 + 335.00 0.1155904 + 340.00 0.1009994 + 345.00 0.8640836E-01 + 350.00 0.7181732E-01 + 355.00 0.6855224E-01 + 360.00 0.6528716E-01 + 365.00 0.6202208E-01 + 370.00 0.5875700E-01 + 375.00 0.5549192E-01 + 380.00 0.5222684E-01 + 385.00 0.4896176E-01 + 390.00 0.4569668E-01 + 395.00 0.4243160E-01 + 400.00 0.3916652E-01 + 405.00 0.3816980E-01 + 410.00 0.3717308E-01 + 415.00 0.3617635E-01 + 420.00 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=================================================================== --- docs/HB5_Expt/ATLAS_1808.00336/fig_02.png (revision 586) +++ docs/HB5_Expt/ATLAS_1808.00336/fig_02.png (revision 587) Property changes on: docs/HB5_Expt/ATLAS_1808.00336/fig_02.png ___________________________________________________________________ Added: svn:mime-type ## -0,0 +1 ## +application/octet-stream \ No newline at end of property Index: docs/HB5_Expt/ATLAS_1807.00539/fig_06a.png =================================================================== Cannot display: file marked as a binary type. svn:mime-type = application/octet-stream Index: docs/HB5_Expt/ATLAS_1807.00539/fig_06a.png =================================================================== --- docs/HB5_Expt/ATLAS_1807.00539/fig_06a.png (revision 586) +++ docs/HB5_Expt/ATLAS_1807.00539/fig_06a.png (revision 587) Property changes on: docs/HB5_Expt/ATLAS_1807.00539/fig_06a.png ___________________________________________________________________ Added: svn:mime-type ## -0,0 +1 ## +application/octet-stream \ No newline at end of property Index: docs/HB5_Expt/ATLAS_1807.00539/exp_interpol.dat =================================================================== --- docs/HB5_Expt/ATLAS_1807.00539/exp_interpol.dat (revision 0) +++ docs/HB5_Expt/ATLAS_1807.00539/exp_interpol.dat (revision 587) @@ -0,0 +1,81 @@ + 20.00 0.2614945E-03 + 20.50 0.2574511E-03 + 21.00 0.2534078E-03 + 21.50 0.2464422E-03 + 22.00 0.2394767E-03 + 22.50 0.2425239E-03 + 23.00 0.2455712E-03 + 23.50 0.2373721E-03 + 24.00 0.2291731E-03 + 24.50 0.2188678E-03 + 25.00 0.2085624E-03 + 25.50 0.2125684E-03 + 26.00 0.2165744E-03 + 26.50 0.2145525E-03 + 27.00 0.2125306E-03 + 27.50 0.2245085E-03 + 28.00 0.2364865E-03 + 28.50 0.2425814E-03 + 29.00 0.2486763E-03 + 29.50 0.2478976E-03 + 30.00 0.2471188E-03 + 30.50 0.2543066E-03 + 31.00 0.2614945E-03 + 31.50 0.2639821E-03 + 32.00 0.2664698E-03 + 32.50 0.2733375E-03 + 33.00 0.2802052E-03 + 33.50 0.2940505E-03 + 34.00 0.3078958E-03 + 34.50 0.3178781E-03 + 35.00 0.3278604E-03 + 35.50 0.3379622E-03 + 36.00 0.3480640E-03 + 36.50 0.3581658E-03 + 37.00 0.3682676E-03 + 37.50 0.3783694E-03 + 38.00 0.3884712E-03 + 38.50 0.3896953E-03 + 39.00 0.3909195E-03 + 39.50 0.4049052E-03 + 40.00 0.4188909E-03 + 40.50 0.4352918E-03 + 41.00 0.4516927E-03 + 41.50 0.4559898E-03 + 42.00 0.4602869E-03 + 42.50 0.4490056E-03 + 43.00 0.4377242E-03 + 43.50 0.4377242E-03 + 44.00 0.4377242E-03 + 44.50 0.4504560E-03 + 45.00 0.4631879E-03 + 45.50 0.4872055E-03 + 46.00 0.5112231E-03 + 46.50 0.5352408E-03 + 47.00 0.5592584E-03 + 47.50 0.5540374E-03 + 48.00 0.5488163E-03 + 48.50 0.5337308E-03 + 49.00 0.5186452E-03 + 49.50 0.5442722E-03 + 50.00 0.5698993E-03 + 50.50 0.5681146E-03 + 51.00 0.5663300E-03 + 51.50 0.5536305E-03 + 52.00 0.5409309E-03 + 52.50 0.5282314E-03 + 53.00 0.5155319E-03 + 53.50 0.5028323E-03 + 54.00 0.4901328E-03 + 54.50 0.4826713E-03 + 55.00 0.4752099E-03 + 55.50 0.4677484E-03 + 56.00 0.4602869E-03 + 56.50 0.4512621E-03 + 57.00 0.4422373E-03 + 57.50 0.4332124E-03 + 58.00 0.4241876E-03 + 58.50 0.4116657E-03 + 59.00 0.3991438E-03 + 59.50 0.3866219E-03 + 60.00 0.3741000E-03 Index: docs/HB5_Expt/ATLAS_1807.00539/data.dat =================================================================== --- docs/HB5_Expt/ATLAS_1807.00539/data.dat (revision 0) +++ docs/HB5_Expt/ATLAS_1807.00539/data.dat (revision 587) @@ -0,0 +1,86 @@ +# ATLAS, arXiv:1807.00539, July 2018, Fig. 6a +# 539_Atlas_H-aa-bbmumu_13TeV_36.1fb-1.txt +# Limit set on SM-normalized sigma(H) x BR(H-> aa -> bbmumu) +# Ma obs exp + + 20.00 0.3258E-03 0.2615E-03 + 20.50 0.3584E-03 0.2575E-03 + 21.00 0.3909E-03 0.2534E-03 + 21.50 0.3533E-03 0.2464E-03 + 22.00 0.3157E-03 0.2395E-03 + 22.50 0.2459E-03 0.2425E-03 + 23.00 0.1760E-03 0.2456E-03 + 23.50 0.1535E-03 0.2374E-03 + 24.00 0.1310E-03 0.2292E-03 + 24.50 0.1249E-03 0.2189E-03 + 25.00 0.1189E-03 0.2086E-03 + 25.50 0.1243E-03 0.2126E-03 + 26.00 0.1298E-03 0.2166E-03 + 26.50 0.1292E-03 0.2146E-03 + 27.00 0.1286E-03 0.2125E-03 + 27.50 0.2144E-03 0.2245E-03 + 28.00 0.3003E-03 0.2365E-03 + 28.50 0.3100E-03 0.2426E-03 + 29.00 0.3197E-03 0.2487E-03 + 29.50 0.2578E-03 0.2479E-03 + 30.00 0.1959E-03 0.2471E-03 + 30.50 0.2385E-03 0.2543E-03 + 31.00 0.2811E-03 0.2615E-03 + 31.50 0.2509E-03 0.2640E-03 + 32.00 0.2207E-03 0.2665E-03 + 32.50 0.2176E-03 0.2733E-03 + 33.00 0.2145E-03 0.2802E-03 + 33.50 0.2215E-03 0.2941E-03 + 34.00 0.2285E-03 0.3079E-03 + 34.50 0.2458E-03 0.3179E-03 + 35.00 0.2631E-03 0.3279E-03 + 35.50 0.3539E-03 0.3380E-03 + 36.00 0.4447E-03 0.3481E-03 + 36.50 0.5164E-03 0.3582E-03 + 37.00 0.5881E-03 0.3683E-03 + 37.50 0.6275E-03 0.3784E-03 + 38.00 0.6668E-03 0.3885E-03 + 38.50 0.5462E-03 0.3897E-03 + 39.00 0.4255E-03 0.3909E-03 + 39.50 0.4688E-03 0.4049E-03 + 40.00 0.5122E-03 0.4189E-03 + 40.50 0.6167E-03 0.4353E-03 + 41.00 0.7213E-03 0.4517E-03 + 41.50 0.7561E-03 0.4560E-03 + 42.00 0.6282E-03 0.4603E-03 + 42.50 0.4971E-03 0.4490E-03 + 43.00 0.3660E-03 0.4377E-03 + 43.50 0.3226E-03 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Index: docs/HB5_Expt/ATLAS_1807.00539/exp.dat =================================================================== --- docs/HB5_Expt/ATLAS_1807.00539/exp.dat (revision 0) +++ docs/HB5_Expt/ATLAS_1807.00539/exp.dat (revision 587) @@ -0,0 +1,33 @@ +20.0 2.6149445432388323E-4 +20.98693759071118 2.53407764770065E-4 +22.00290275761974 2.3947672017289912E-4 +22.989840348330915 2.4557115527285424E-4 +24.00580551523948 2.2917313764310893E-4 +24.99274310595065 2.0856240029032717E-4 +26.008708272859216 2.1657438715148316E-4 +26.995645863570395 2.1253064255706742E-4 +28.011611030478953 2.3648645742190835E-4 +28.99854862119013 2.486762898599909E-4 +29.98548621190131 2.4711884547699945E-4 +31.00145137880987 2.6149445432388323E-4 +31.988388969521047 2.664698158690214E-4 +33.00435413642961 2.8020515801360367E-4 +34.02031930333817 3.078958391175499E-4 +35.00725689404935 3.278603887707404E-4 +37.99709724238026 3.8847117523523815E-4 +39.042089985486214 3.909194800120607E-4 +40.0 4.1889092811009827E-4 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0.5606200E-03 + 47.00 0.6106772E-03 + 47.50 0.6294562E-03 + 48.00 0.6482352E-03 + 48.50 0.6472186E-03 + 49.00 0.6462021E-03 + 49.50 0.7517694E-03 + 50.00 0.8573367E-03 + 50.50 0.8654544E-03 + 51.00 0.7876196E-03 + 51.50 0.6991484E-03 + 52.00 0.6106772E-03 + 52.50 0.5147841E-03 + 53.00 0.4188909E-03 + 53.50 0.3581647E-03 + 54.00 0.2974384E-03 + 54.50 0.2923872E-03 + 55.00 0.2873361E-03 + 55.50 0.3011880E-03 + 56.00 0.3150400E-03 + 56.50 0.3288919E-03 + 57.00 0.3503890E-03 + 57.50 0.3718861E-03 + 58.00 0.3933832E-03 + 58.50 0.3885018E-03 + 59.00 0.3836205E-03 + 59.50 0.3599123E-03 + 60.00 0.3362041E-03 Index: docs/HB5_Expt/ATLAS_1807.00539/obs.dat =================================================================== --- docs/HB5_Expt/ATLAS_1807.00539/obs.dat (revision 0) +++ docs/HB5_Expt/ATLAS_1807.00539/obs.dat (revision 587) @@ -0,0 +1,44 @@ +20.0 3.258070192227879E-4 +20.98693759071118 3.909194800120607E-4 +22.00290275761974 3.15731470103699E-4 +23.0188679245283 1.7602168191948475E-4 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___________________________________________________________________ Added: svn:mime-type ## -0,0 +1 ## +application/octet-stream \ No newline at end of property Index: docs/HB5_Expt/ATLAS_1809.06682/data.dat =================================================================== --- docs/HB5_Expt/ATLAS_1809.06682/data.dat (revision 0) +++ docs/HB5_Expt/ATLAS_1809.06682/data.dat (revision 587) @@ -0,0 +1,591 @@ +# ATLAS, arXiv:1809.06682, Sept. 2018, Fig. 6b +# 6682_Atlas_VBF_h-invisible_13TeV_36.1fb-1.txt +# Limit set on sigma(h,VBF) x BR(h->inv) in pb +# Mh obs exp + + 75.00 1.979 1.502 + 80.00 1.942 1.473 + 85.00 1.905 1.444 + 90.00 1.867 1.414 + 95.00 1.830 1.385 + 100.0 1.793 1.356 + 105.0 1.756 1.327 + 110.0 1.719 1.298 + 115.0 1.681 1.269 + 120.0 1.644 1.240 + 125.0 1.607 1.211 + 130.0 1.586 1.195 + 135.0 1.565 1.180 + 140.0 1.544 1.165 + 145.0 1.523 1.149 + 150.0 1.502 1.134 + 155.0 1.481 1.118 + 160.0 1.460 1.103 + 165.0 1.439 1.088 + 170.0 1.418 1.072 + 175.0 1.397 1.057 + 180.0 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docs/HB5_Expt/ATLAS_1809.06682/obs_interpol.dat =================================================================== --- docs/HB5_Expt/ATLAS_1809.06682/obs_interpol.dat (revision 0) +++ docs/HB5_Expt/ATLAS_1809.06682/obs_interpol.dat (revision 587) @@ -0,0 +1,586 @@ + 75.00 1.978947 + 80.00 1.941754 + 85.00 1.904561 + 90.00 1.867368 + 95.00 1.830175 + 100.00 1.792982 + 105.00 1.755789 + 110.00 1.718596 + 115.00 1.681404 + 120.00 1.644211 + 125.00 1.607018 + 130.00 1.586065 + 135.00 1.565113 + 140.00 1.544160 + 145.00 1.523208 + 150.00 1.502256 + 155.00 1.481303 + 160.00 1.460351 + 165.00 1.439398 + 170.00 1.418446 + 175.00 1.397494 + 180.00 1.376541 + 185.00 1.355589 + 190.00 1.334637 + 195.00 1.313684 + 200.00 1.292732 + 205.00 1.271779 + 210.00 1.250827 + 215.00 1.229875 + 220.00 1.208922 + 225.00 1.187970 + 230.00 1.167018 + 235.00 1.146065 + 240.00 1.125113 + 245.00 1.104160 + 250.00 1.083208 + 255.00 1.062256 + 260.00 1.041303 + 265.00 1.020351 + 270.00 0.9993985 + 275.00 0.9784461 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0.5403481E-02 + 446.00 0.5383206E-02 + 447.00 0.5362931E-02 + 448.00 0.5342656E-02 + 449.00 0.5322381E-02 + 450.00 0.5302106E-02 + 451.00 0.5281831E-02 + 452.00 0.5261557E-02 + 453.00 0.5241282E-02 + 454.00 0.5221007E-02 + 455.00 0.5200732E-02 + 456.00 0.5180457E-02 + 457.00 0.5160182E-02 + 458.00 0.5139907E-02 + 459.00 0.5119632E-02 + 460.00 0.5099358E-02 + 461.00 0.5079083E-02 + 462.00 0.5058808E-02 + 463.00 0.5038533E-02 + 464.00 0.5018258E-02 + 465.00 0.4997983E-02 + 466.00 0.4977708E-02 + 467.00 0.4957433E-02 + 468.00 0.4937159E-02 + 469.00 0.4916884E-02 + 470.00 0.4896609E-02 + 471.00 0.4876334E-02 + 472.00 0.4856059E-02 + 473.00 0.4835784E-02 + 474.00 0.4815509E-02 + 475.00 0.4795234E-02 + 476.00 0.4774960E-02 + 477.00 0.4754685E-02 + 478.00 0.4734410E-02 + 479.00 0.4714135E-02 + 480.00 0.4693860E-02 + 481.00 0.4673585E-02 + 482.00 0.4653310E-02 + 483.00 0.4633036E-02 + 484.00 0.4612761E-02 + 485.00 0.4592486E-02 + 486.00 0.4572211E-02 + 487.00 0.4551936E-02 + 488.00 0.4531661E-02 + 489.00 0.4511386E-02 + 490.00 0.4491111E-02 + 491.00 0.4470837E-02 + 492.00 0.4450562E-02 + 493.00 0.4430287E-02 + 494.00 0.4410012E-02 + 495.00 0.4389737E-02 + 496.00 0.4369462E-02 + 497.00 0.4349187E-02 + 498.00 0.4328912E-02 + 499.00 0.4308638E-02 + 500.00 0.4288363E-02 Index: docs/HB5_Expt/ATLAS_1807.08567/data.dat =================================================================== --- docs/HB5_Expt/ATLAS_1807.08567/data.dat (revision 0) +++ docs/HB5_Expt/ATLAS_1807.08567/data.dat (revision 587) @@ -0,0 +1,246 @@ +# ATLAS, arXiv:1807.08567, July 2018, Fig. 4b +# 8567_Atlas_X-HH-WWgaga_13TeV_36.1fb-1.txt +# limit set on sigma(pp->X) x BR(X->HH) x BR(H->WW) x BR(H->gaga) x 2 [symmetryfactor] in pb +# MX obs exp + + 260.0 0.3944E-01 0.1726E-01 + 261.0 0.3928E-01 0.1720E-01 + 262.0 0.3912E-01 0.1713E-01 + 263.0 0.3896E-01 0.1707E-01 + 264.0 0.3879E-01 0.1700E-01 + 265.0 0.3863E-01 0.1694E-01 + 266.0 0.3847E-01 0.1687E-01 + 267.0 0.3831E-01 0.1681E-01 + 268.0 0.3814E-01 0.1674E-01 + 269.0 0.3798E-01 0.1667E-01 + 270.0 0.3782E-01 0.1661E-01 + 271.0 0.3766E-01 0.1654E-01 + 272.0 0.3750E-01 0.1648E-01 + 273.0 0.3733E-01 0.1641E-01 + 274.0 0.3717E-01 0.1635E-01 + 275.0 0.3701E-01 0.1628E-01 + 276.0 0.3685E-01 0.1622E-01 + 277.0 0.3668E-01 0.1615E-01 + 278.0 0.3652E-01 0.1609E-01 + 279.0 0.3636E-01 0.1602E-01 + 280.0 0.3620E-01 0.1596E-01 + 281.0 0.3604E-01 0.1589E-01 + 282.0 0.3587E-01 0.1583E-01 + 283.0 0.3571E-01 0.1576E-01 + 284.0 0.3555E-01 0.1570E-01 + 285.0 0.3539E-01 0.1563E-01 + 286.0 0.3522E-01 0.1556E-01 + 287.0 0.3506E-01 0.1550E-01 + 288.0 0.3490E-01 0.1543E-01 + 289.0 0.3474E-01 0.1537E-01 + 290.0 0.3458E-01 0.1530E-01 + 291.0 0.3441E-01 0.1524E-01 + 292.0 0.3425E-01 0.1517E-01 + 293.0 0.3409E-01 0.1511E-01 + 294.0 0.3393E-01 0.1504E-01 + 295.0 0.3376E-01 0.1498E-01 + 296.0 0.3360E-01 0.1491E-01 + 297.0 0.3344E-01 0.1485E-01 + 298.0 0.3328E-01 0.1478E-01 + 299.0 0.3312E-01 0.1472E-01 + 300.0 0.3295E-01 0.1465E-01 + 301.0 0.3279E-01 0.1459E-01 + 302.0 0.3263E-01 0.1452E-01 + 303.0 0.3247E-01 0.1446E-01 + 304.0 0.3230E-01 0.1439E-01 + 305.0 0.3214E-01 0.1432E-01 + 306.0 0.3198E-01 0.1426E-01 + 307.0 0.3182E-01 0.1419E-01 + 308.0 0.3166E-01 0.1413E-01 + 309.0 0.3149E-01 0.1406E-01 + 310.0 0.3133E-01 0.1400E-01 + 311.0 0.3117E-01 0.1393E-01 + 312.0 0.3101E-01 0.1387E-01 + 313.0 0.3084E-01 0.1380E-01 + 314.0 0.3068E-01 0.1374E-01 + 315.0 0.3052E-01 0.1367E-01 + 316.0 0.3036E-01 0.1361E-01 + 317.0 0.3020E-01 0.1354E-01 + 318.0 0.3003E-01 0.1348E-01 + 319.0 0.2987E-01 0.1341E-01 + 320.0 0.2971E-01 0.1335E-01 + 321.0 0.2955E-01 0.1328E-01 + 322.0 0.2938E-01 0.1321E-01 + 323.0 0.2922E-01 0.1315E-01 + 324.0 0.2906E-01 0.1308E-01 + 325.0 0.2890E-01 0.1302E-01 + 326.0 0.2874E-01 0.1295E-01 + 327.0 0.2857E-01 0.1289E-01 + 328.0 0.2841E-01 0.1282E-01 + 329.0 0.2825E-01 0.1276E-01 + 330.0 0.2809E-01 0.1269E-01 + 331.0 0.2792E-01 0.1263E-01 + 332.0 0.2776E-01 0.1256E-01 + 333.0 0.2760E-01 0.1250E-01 + 334.0 0.2744E-01 0.1243E-01 + 335.0 0.2728E-01 0.1237E-01 + 336.0 0.2711E-01 0.1230E-01 + 337.0 0.2695E-01 0.1224E-01 + 338.0 0.2679E-01 0.1217E-01 + 339.0 0.2663E-01 0.1211E-01 + 340.0 0.2646E-01 0.1204E-01 + 341.0 0.2630E-01 0.1197E-01 + 342.0 0.2614E-01 0.1191E-01 + 343.0 0.2598E-01 0.1184E-01 + 344.0 0.2582E-01 0.1178E-01 + 345.0 0.2565E-01 0.1171E-01 + 346.0 0.2549E-01 0.1165E-01 + 347.0 0.2533E-01 0.1158E-01 + 348.0 0.2517E-01 0.1152E-01 + 349.0 0.2500E-01 0.1145E-01 + 350.0 0.2484E-01 0.1139E-01 + 351.0 0.2474E-01 0.1134E-01 + 352.0 0.2465E-01 0.1130E-01 + 353.0 0.2455E-01 0.1126E-01 + 354.0 0.2445E-01 0.1122E-01 + 355.0 0.2435E-01 0.1117E-01 + 356.0 0.2426E-01 0.1113E-01 + 357.0 0.2416E-01 0.1109E-01 + 358.0 0.2406E-01 0.1105E-01 + 359.0 0.2396E-01 0.1100E-01 + 360.0 0.2387E-01 0.1096E-01 + 361.0 0.2377E-01 0.1092E-01 + 362.0 0.2367E-01 0.1088E-01 + 363.0 0.2357E-01 0.1083E-01 + 364.0 0.2348E-01 0.1079E-01 + 365.0 0.2338E-01 0.1075E-01 + 366.0 0.2328E-01 0.1071E-01 + 367.0 0.2318E-01 0.1066E-01 + 368.0 0.2309E-01 0.1062E-01 + 369.0 0.2299E-01 0.1058E-01 + 370.0 0.2289E-01 0.1054E-01 + 371.0 0.2279E-01 0.1049E-01 + 372.0 0.2270E-01 0.1045E-01 + 373.0 0.2260E-01 0.1041E-01 + 374.0 0.2250E-01 0.1037E-01 + 375.0 0.2240E-01 0.1032E-01 + 376.0 0.2231E-01 0.1028E-01 + 377.0 0.2221E-01 0.1024E-01 + 378.0 0.2211E-01 0.1020E-01 + 379.0 0.2201E-01 0.1015E-01 + 380.0 0.2191E-01 0.1011E-01 + 381.0 0.2182E-01 0.1007E-01 + 382.0 0.2172E-01 0.1003E-01 + 383.0 0.2162E-01 0.9983E-02 + 384.0 0.2152E-01 0.9940E-02 + 385.0 0.2143E-01 0.9898E-02 + 386.0 0.2133E-01 0.9855E-02 + 387.0 0.2123E-01 0.9813E-02 + 388.0 0.2113E-01 0.9770E-02 + 389.0 0.2104E-01 0.9727E-02 + 390.0 0.2094E-01 0.9685E-02 + 391.0 0.2084E-01 0.9642E-02 + 392.0 0.2074E-01 0.9600E-02 + 393.0 0.2065E-01 0.9557E-02 + 394.0 0.2055E-01 0.9515E-02 + 395.0 0.2045E-01 0.9472E-02 + 396.0 0.2035E-01 0.9430E-02 + 397.0 0.2026E-01 0.9387E-02 + 398.0 0.2016E-01 0.9344E-02 + 399.0 0.2006E-01 0.9302E-02 + 400.0 0.9142E-02 0.6316E-02 + 401.0 0.9111E-02 0.6296E-02 + 402.0 0.9080E-02 0.6275E-02 + 403.0 0.9049E-02 0.6255E-02 + 404.0 0.9018E-02 0.6235E-02 + 405.0 0.8986E-02 0.6214E-02 + 406.0 0.8955E-02 0.6194E-02 + 407.0 0.8924E-02 0.6174E-02 + 408.0 0.8893E-02 0.6154E-02 + 409.0 0.8862E-02 0.6133E-02 + 410.0 0.8831E-02 0.6113E-02 + 411.0 0.8800E-02 0.6093E-02 + 412.0 0.8769E-02 0.6073E-02 + 413.0 0.8738E-02 0.6052E-02 + 414.0 0.8706E-02 0.6032E-02 + 415.0 0.8675E-02 0.6012E-02 + 416.0 0.8644E-02 0.5991E-02 + 417.0 0.8613E-02 0.5971E-02 + 418.0 0.8582E-02 0.5951E-02 + 419.0 0.8551E-02 0.5931E-02 + 420.0 0.8520E-02 0.5910E-02 + 421.0 0.8489E-02 0.5890E-02 + 422.0 0.8458E-02 0.5870E-02 + 423.0 0.8426E-02 0.5850E-02 + 424.0 0.8395E-02 0.5829E-02 + 425.0 0.8364E-02 0.5809E-02 + 426.0 0.8333E-02 0.5789E-02 + 427.0 0.8302E-02 0.5768E-02 + 428.0 0.8271E-02 0.5748E-02 + 429.0 0.8240E-02 0.5728E-02 + 430.0 0.8209E-02 0.5708E-02 + 431.0 0.8177E-02 0.5687E-02 + 432.0 0.8146E-02 0.5667E-02 + 433.0 0.8115E-02 0.5647E-02 + 434.0 0.8084E-02 0.5627E-02 + 435.0 0.8053E-02 0.5606E-02 + 436.0 0.8022E-02 0.5586E-02 + 437.0 0.7991E-02 0.5566E-02 + 438.0 0.7960E-02 0.5545E-02 + 439.0 0.7929E-02 0.5525E-02 + 440.0 0.7897E-02 0.5505E-02 + 441.0 0.7866E-02 0.5485E-02 + 442.0 0.7835E-02 0.5464E-02 + 443.0 0.7804E-02 0.5444E-02 + 444.0 0.7773E-02 0.5424E-02 + 445.0 0.7742E-02 0.5403E-02 + 446.0 0.7711E-02 0.5383E-02 + 447.0 0.7680E-02 0.5363E-02 + 448.0 0.7649E-02 0.5343E-02 + 449.0 0.7617E-02 0.5322E-02 + 450.0 0.7586E-02 0.5302E-02 + 451.0 0.7555E-02 0.5282E-02 + 452.0 0.7524E-02 0.5262E-02 + 453.0 0.7493E-02 0.5241E-02 + 454.0 0.7462E-02 0.5221E-02 + 455.0 0.7431E-02 0.5201E-02 + 456.0 0.7400E-02 0.5180E-02 + 457.0 0.7368E-02 0.5160E-02 + 458.0 0.7337E-02 0.5140E-02 + 459.0 0.7306E-02 0.5120E-02 + 460.0 0.7275E-02 0.5099E-02 + 461.0 0.7244E-02 0.5079E-02 + 462.0 0.7213E-02 0.5059E-02 + 463.0 0.7182E-02 0.5039E-02 + 464.0 0.7151E-02 0.5018E-02 + 465.0 0.7120E-02 0.4998E-02 + 466.0 0.7088E-02 0.4978E-02 + 467.0 0.7057E-02 0.4957E-02 + 468.0 0.7026E-02 0.4937E-02 + 469.0 0.6995E-02 0.4917E-02 + 470.0 0.6964E-02 0.4897E-02 + 471.0 0.6933E-02 0.4876E-02 + 472.0 0.6902E-02 0.4856E-02 + 473.0 0.6871E-02 0.4836E-02 + 474.0 0.6840E-02 0.4816E-02 + 475.0 0.6808E-02 0.4795E-02 + 476.0 0.6777E-02 0.4775E-02 + 477.0 0.6746E-02 0.4755E-02 + 478.0 0.6715E-02 0.4734E-02 + 479.0 0.6684E-02 0.4714E-02 + 480.0 0.6653E-02 0.4694E-02 + 481.0 0.6622E-02 0.4674E-02 + 482.0 0.6591E-02 0.4653E-02 + 483.0 0.6559E-02 0.4633E-02 + 484.0 0.6528E-02 0.4613E-02 + 485.0 0.6497E-02 0.4592E-02 + 486.0 0.6466E-02 0.4572E-02 + 487.0 0.6435E-02 0.4552E-02 + 488.0 0.6404E-02 0.4532E-02 + 489.0 0.6373E-02 0.4511E-02 + 490.0 0.6342E-02 0.4491E-02 + 491.0 0.6311E-02 0.4471E-02 + 492.0 0.6279E-02 0.4451E-02 + 493.0 0.6248E-02 0.4430E-02 + 494.0 0.6217E-02 0.4410E-02 + 495.0 0.6186E-02 0.4390E-02 + 496.0 0.6155E-02 0.4369E-02 + 497.0 0.6124E-02 0.4349E-02 + 498.0 0.6093E-02 0.4329E-02 + 499.0 0.6062E-02 0.4309E-02 + 500.0 0.6031E-02 0.4288E-02 Index: docs/HB5_Expt/ATLAS_1807.08567/exp.dat =================================================================== --- docs/HB5_Expt/ATLAS_1807.08567/exp.dat (revision 0) +++ docs/HB5_Expt/ATLAS_1807.08567/exp.dat (revision 587) @@ -0,0 +1,5 @@ +259.8438560760353 0.017262143000910033 +349.96605566870335 0.01138692905990197 +399.0156143923965 0.009301909811296607 +400.03394433129665 0.0063158500976385635 +499.66055668703325 0.004288362633595642 Index: docs/HB5_Expt/ATLAS_1807.08567/obs_interpol.dat =================================================================== --- docs/HB5_Expt/ATLAS_1807.08567/obs_interpol.dat (revision 0) +++ docs/HB5_Expt/ATLAS_1807.08567/obs_interpol.dat (revision 587) @@ -0,0 +1,241 @@ + 260.00 0.3944222E-01 + 261.00 0.3928000E-01 + 262.00 0.3911778E-01 + 263.00 0.3895556E-01 + 264.00 0.3879335E-01 + 265.00 0.3863113E-01 + 266.00 0.3846891E-01 + 267.00 0.3830669E-01 + 268.00 0.3814447E-01 + 269.00 0.3798226E-01 + 270.00 0.3782004E-01 + 271.00 0.3765782E-01 + 272.00 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0.7772979E-02 + 445.00 0.7741864E-02 + 446.00 0.7710748E-02 + 447.00 0.7679633E-02 + 448.00 0.7648518E-02 + 449.00 0.7617403E-02 + 450.00 0.7586288E-02 + 451.00 0.7555172E-02 + 452.00 0.7524057E-02 + 453.00 0.7492942E-02 + 454.00 0.7461827E-02 + 455.00 0.7430712E-02 + 456.00 0.7399597E-02 + 457.00 0.7368481E-02 + 458.00 0.7337366E-02 + 459.00 0.7306251E-02 + 460.00 0.7275136E-02 + 461.00 0.7244021E-02 + 462.00 0.7212905E-02 + 463.00 0.7181790E-02 + 464.00 0.7150675E-02 + 465.00 0.7119560E-02 + 466.00 0.7088445E-02 + 467.00 0.7057329E-02 + 468.00 0.7026214E-02 + 469.00 0.6995099E-02 + 470.00 0.6963984E-02 + 471.00 0.6932869E-02 + 472.00 0.6901754E-02 + 473.00 0.6870638E-02 + 474.00 0.6839523E-02 + 475.00 0.6808408E-02 + 476.00 0.6777293E-02 + 477.00 0.6746178E-02 + 478.00 0.6715062E-02 + 479.00 0.6683947E-02 + 480.00 0.6652832E-02 + 481.00 0.6621717E-02 + 482.00 0.6590602E-02 + 483.00 0.6559486E-02 + 484.00 0.6528371E-02 + 485.00 0.6497256E-02 + 486.00 0.6466141E-02 + 487.00 0.6435026E-02 + 488.00 0.6403911E-02 + 489.00 0.6372795E-02 + 490.00 0.6341680E-02 + 491.00 0.6310565E-02 + 492.00 0.6279450E-02 + 493.00 0.6248335E-02 + 494.00 0.6217219E-02 + 495.00 0.6186104E-02 + 496.00 0.6154989E-02 + 497.00 0.6123874E-02 + 498.00 0.6092759E-02 + 499.00 0.6061643E-02 + 500.00 0.6030528E-02 Index: trunk/HiggsBounds-5/S95tables.f90 =================================================================== --- trunk/HiggsBounds-5/S95tables.f90 (revision 586) +++ trunk/HiggsBounds-5/S95tables.f90 (revision 587) @@ -1,5182 +1,5256 @@ ! This file is part of HiggsBounds ! -KW !****************************************************************** module S95tables !****************************************************************** use S95tables_type1 use S95tables_type2 use usefulbits, only: Hneut,Hplus implicit none private public :: & & S95_t1,S95_t2, & & setup_S95tables,deallocate_S95tables, & & calcfact,outputproc, & & check_against_bound, & & convolve_chisq_with_gaussian, & & S95_t1_or_S95_t2_idfromelementnumber, & & f_from_t2,f_from_t3,f_from_slices_t2, & & WhichColliderString,get_collider_element_number, & & inrange, deallocate_Exptranges integer :: ntable1,ntable2 !----------------------------------------------------------------------------------- ! delta_M*_* determine how close in mass particles should be before their masses are combined ! nb. delta*_* is only used for tables of type 1 at the moment ! for some analyses, S95_t1(x)%deltax has already been set in S95tables_type1.f90 ! for analyses where S95_t1(x)%deltax is *not* has already set: ! we set ! LEP neutral Higgs tables to have deltax=delta_Mh_LEP ! Tevatron neutral Higgs tables to have deltax=delta_Mh_TEV ! LHC neutral Higgs tables to have deltax=delta_Mh_LHC ! LEP charged Higgs tables to have deltax=delta_Mhplus_LEP ! Tevatron charged Higgs tables to have deltax=delta_Mhplus_TEV ! LHC charged Higgs tables to have deltax=delta_Mhplus_LHC ! other LEP tables to have deltax=delta_M_LEP_default ! other Tevatron tables to have deltax=delta_M_TEV_default ! other LHC tables to have deltax=delta_M_LHC_default ! setting delta_M*_LHC and/or delta_M*_TEV and/or delta_M*_LEP to zero turns this feature off ! DO NOT CHANGE THESE VALUES BEFORE READING THE MANUAL ! even when it is appropriate to add the cross sections, we would recommend using ! delta_Mh_LEP<=2.0D0, delta_Mh_TEV<=10.0, delta_Mh_LHC<=10.0 double precision, parameter :: delta_Mh_LEP=0.0D0 double precision, parameter :: delta_Mh_TEV=10.0D0 double precision, parameter :: delta_Mh_LHC=10.0D0 double precision, parameter :: delta_Mhplus_LEP=0.0D0 double precision, parameter :: delta_Mhplus_TEV=0.0D0 double precision, parameter :: delta_Mhplus_LHC=0.0D0 double precision, parameter :: delta_M_LEP_default=0.0D0 !where delta_M_LEP/TEV/LHC is not specified double precision, parameter :: delta_M_TEV_default=0.0D0 !these values will be used double precision, parameter :: delta_M_LHC_default=0.0D0 ! !double precision, parameter :: delta_Mh_LEP=15.0D0 !crazy values - for debugging only !double precision, parameter :: delta_Mh_TEV=15.0D0 !crazy(ish) values - for debugging only !double precision, parameter :: delta_Mh_LHC=15.0D0 !crazy(ish) values - for debugging only !----------------------------------------------------------------------------------- ! Use the SM expected channel contributions to weight the channels in the likeness test logical :: use_weight = .True. ! eps determines how strict the Standard Model test is double precision, parameter :: eps=2.0D-2 !double precision, parameter :: eps=1.0D3 !crazy value - for debugging only !----------------------------------------------------------------------------------- !table type 1----------------------------- type(table1),allocatable :: S95_t1(:) !------------------------------------------ !table type 2------------------------------ type(table2),allocatable :: S95_t2(:) !------------------------------------------ character(LEN=5),parameter :: colliders(5) = (/'LEP ','TEV ','LHC7 ','LHC8 ','LHC13'/) !------------------------------------------- double precision, allocatable :: Exptrange_Mhmin_forSMdecays(:), Exptrange_Mhmax_forSMdecays(:) double precision, allocatable :: Exptrange_Mhmin_forSMXS(:), Exptrange_Mhmax_forSMXS(:) contains !********************************************************** subroutine setup_S95tables ! Allocates and calls subroutines to fill S95_t1, S95_t2 ! (which store the experimental data) ! Sets delta_M_TEV,delta_M_LEP,delta_M_LHC which govern how close Higgs ! need to be in mass before HiggsBounds combines their cross sections !********************************************************** use usefulbits, only : debug,np,not_a_particle use theory_BRfunctions, only : BRSMt1Mhmax,BRSMt1Mhmin use theory_XS_SM_functions, only : tevXS_SM_functions_xmin, tevXS_SM_functions_xmax, & & lhc7XS_SM_functions_xmin,lhc7XS_SM_functions_xmax, & & lhc8XS_SM_functions_xmin,lhc8XS_SM_functions_xmax, & & lhc13XS_SM_functions_xmin,lhc13XS_SM_functions_xmax implicit none !-----------------------------------internal integer :: i,c double precision, allocatable :: max_expt_delta_Mh(:) double precision, allocatable :: Expttables_Mhmin_forSMXS(:),Expttables_Mhmax_forSMXS(:) double precision, allocatable :: Expttables_Mhmin_forSMdecays(:),Expttables_Mhmax_forSMdecays(:) double precision, allocatable :: delta_x_default(:,:) ! these numbers have to be changed appropriately every time a table is added ! or taken away: - ntable1=195 + ntable1=201 ntable2=37 ! table type 2 involves 2 variables allocate(S95_t1(ntable1)) allocate(S95_t2(ntable2)) call initializetables_type1_blank(S95_t1) call initializetables_type2_blank(S95_t2) call initializetables1(S95_t1) call initializetables2(S95_t2) allocate( Expttables_Mhmin_forSMXS( size(colliders,dim=1) ) ) allocate( Expttables_Mhmax_forSMXS( size(colliders,dim=1) ) ) allocate( Exptrange_Mhmin_forSMXS( size(colliders,dim=1) ) ) allocate( Exptrange_Mhmax_forSMXS( size(colliders,dim=1) ) ) allocate( Expttables_Mhmin_forSMdecays( size(colliders,dim=1) ) ) allocate( Expttables_Mhmax_forSMdecays( size(colliders,dim=1) ) ) allocate( Exptrange_Mhmin_forSMdecays( size(colliders,dim=1) ) ) allocate( Exptrange_Mhmax_forSMdecays( size(colliders,dim=1) ) ) allocate( max_expt_delta_Mh( size(colliders,dim=1) ) ) ! will pick up on any typos in S95_t1%expt do i=lbound(S95_t1,dim=1),ubound(S95_t1,dim=1) if(WhichColliderElement(S95_t1(i)%expt, S95_t1(i)%energy).eq.0)then write(*,*)'~'//trim(adjustl(S95_t1(i)%expt))//'~ is not a valid experiment name' stop 'error in setup_S95tables (a)' endif enddo ! will pick up on any typos in S95_t2%expt do i=lbound(S95_t2,dim=1),ubound(S95_t2,dim=1) if(WhichColliderElement(S95_t2(i)%expt, S95_t2(i)%energy).eq.0)then write(*,*)'~'//trim(adjustl(S95_t2(i)%expt))//'~ is not a valid experiment name' stop 'error in setup_S95tables (b)' endif enddo ! checks that none of the id's are repeated in S95_t1 do i=lbound(S95_t1,dim=1),ubound(S95_t1,dim=1) if( count(S95_t1%id.eq.S95_t1(i)%id) & +count(S95_t2%id.eq.S95_t1(i)%id).ne.1)then write(*,*)'the id',S95_t1(i)%id,'is repeated' stop 'error in setup_S95tables (c1)' endif enddo ! checks that none of the id's are repeated in S95_t2 do i=lbound(S95_t2,dim=1),ubound(S95_t2,dim=1) if( count(S95_t1%id.eq.S95_t2(i)%id)& +count(S95_t2%id.eq.S95_t2(i)%id).ne.1)then write(*,*)'the id',S95_t2(i)%id,'is repeated' stop 'error in setup_S95tables (c2)' endif enddo !check to make sure that S95_t1(i)%particle_x are all particles do i=lbound(S95_t1,dim=1),ubound(S95_t1,dim=1) if(S95_t1(i)%particle_x.eq.not_a_particle)then write(*,*)S95_t1(i)%id,'particle_x=not_a_particle.' stop 'error in setup_S95tables (d1)' endif enddo !check to make sure that S95_t2(i)%particle_x2 are all particles do i=lbound(S95_t2,dim=1),ubound(S95_t2,dim=1) if(S95_t2(i)%particle_x2.eq.not_a_particle)then write(*,*)S95_t2(i)%id,'particle_x2=not_a_particle.' stop 'error in setup_S95tables (d2)' endif enddo ! looks for the min and max values of Mh (neutral Higgs) in each type of tables ! will be used in input.f90 to work out which SM para need to be calculated ! initial (impossible) values Expttables_Mhmin_forSMXS=1.0D6 Expttables_Mhmax_forSMXS=0.0D0 do i=lbound(S95_t1,dim=1),ubound(S95_t1,dim=1) if(S95_t1(i)%particle_x.eq.Hneut)then do c=1,ubound(colliders,dim=1) if(WhichColliderElement(S95_t1(i)%expt, S95_t1(i)%energy).eq.c)then if(S95_t1(i)%xmax.gt.Expttables_Mhmax_forSMXS(c))Expttables_Mhmax_forSMXS(c)=S95_t1(i)%xmax if(S95_t1(i)%xmin.lt.Expttables_Mhmin_forSMXS(c))Expttables_Mhmin_forSMXS(c)=S95_t1(i)%xmin endif enddo endif enddo do i=lbound(S95_t2,dim=1),ubound(S95_t2,dim=1) if(S95_t2(i)%particle_x2.eq.Hneut)then do c=1,ubound(colliders,dim=1) if(WhichColliderElement(S95_t2(i)%expt, S95_t2(i)%energy).eq.c)then if(S95_t2(i)%xmax2.gt.Expttables_Mhmax_forSMdecays(c))Expttables_Mhmax_forSMdecays(c)=S95_t2(i)%xmax2 if(S95_t2(i)%xmin2.lt.Expttables_Mhmin_forSMdecays(c))Expttables_Mhmin_forSMdecays(c)=S95_t2(i)%xmin2 endif enddo endif enddo Expttables_Mhmin_forSMdecays=Expttables_Mhmin_forSMXS Expttables_Mhmax_forSMdecays=Expttables_Mhmax_forSMXS do i=lbound(S95_t2,dim=1),ubound(S95_t2,dim=1) if(S95_t2(i)%particle_x1.eq.Hneut)then do c=1,ubound(colliders,dim=1) if(WhichColliderElement(S95_t2(i)%expt, S95_t2(i)%energy).eq.c)then if(S95_t2(i)%xmax1.gt.Expttables_Mhmax_forSMdecays(c))Expttables_Mhmax_forSMdecays(c)=S95_t2(i)%xmax1 if(S95_t2(i)%xmin1.lt.Expttables_Mhmin_forSMdecays(c))Expttables_Mhmin_forSMdecays(c)=S95_t2(i)%xmin1 ! Needs_M2_gt_2M1 is true only for processes involving hj->hihi. ! Therefore, SM production cross sections will not be needed for hi. if(.not.S95_t2(i)%needs_M2_gt_2M1)then if(S95_t2(i)%xmax1.gt.Expttables_Mhmax_forSMXS(c))Expttables_Mhmax_forSMXS(c)=S95_t2(i)%xmax1 if(S95_t2(i)%xmin1.lt.Expttables_Mhmin_forSMXS(c))Expttables_Mhmin_forSMXS(c)=S95_t2(i)%xmin1 else if(S95_t2(i)%xmax2.gt.Expttables_Mhmax_forSMXS(c))Expttables_Mhmax_forSMXS(c)=S95_t2(i)%xmax2 if(S95_t2(i)%xmin2.lt.Expttables_Mhmin_forSMXS(c))Expttables_Mhmin_forSMXS(c)=S95_t2(i)%xmin2 endif endif enddo endif enddo ! now we set delta_x if(delta_M_LEP_default.gt.2.1d0) write(*,*)'WARNING: delta_M_LEP_default.gt.2.1d0' if(delta_M_TEV_default.gt.10.1d0)write(*,*)'WARNING: delta_M_TEV_default.gt.10.1d0' if(delta_M_LHC_default.gt.10.1d0)write(*,*)'WARNING: delta_M_LHC_default.gt.10.1d0' if(delta_Mh_LEP .gt.2.1d0) write(*,*)'WARNING: delta_Mh_LEP.gt.2.1d0' if(delta_Mh_TEV .gt.10.1d0)write(*,*)'WARNING: delta_Mh_TEV.gt.10.1d0' if(delta_Mh_LHC .gt.10.1d0)write(*,*)'WARNING: delta_Mh_LHC.gt.10.1d0' if(delta_Mhplus_LEP .gt.2.1d0) write(*,*)'WARNING: delta_Mhplus_LEP.gt.2.1d0' if(delta_Mhplus_TEV .gt.10.1d0)write(*,*)'WARNING: delta_Mhplus_TEV.gt.10.1d0' if(delta_Mhplus_LHC .gt.10.1d0)write(*,*)'WARNING: delta_Mhplus_LHC.gt.10.1d0' allocate( delta_x_default(size(np,dim=1),size(colliders,dim=1)) ) ! fill delta_x_default do c=1,ubound(colliders,dim=1) if(c.eq.get_collider_element_number('LEP '))then ! for some reason, gfortran didn't like having a case statement here delta_x_default(:,c) =delta_M_LEP_default delta_x_default(Hneut,c)=delta_Mh_LEP delta_x_default(Hplus,c)=delta_Mhplus_LEP elseif(c.eq.get_collider_element_number('TEV '))then delta_x_default(:,c) =delta_M_TEV_default delta_x_default(Hneut,c)=delta_Mh_TEV delta_x_default(Hplus,c)=delta_Mhplus_TEV elseif(c.eq.get_collider_element_number('LHC7 '))then delta_x_default(:,c) =delta_M_LHC_default delta_x_default(Hneut,c)=delta_Mh_LHC delta_x_default(Hplus,c)=delta_Mhplus_LHC elseif(c.eq.get_collider_element_number('LHC8 '))then delta_x_default(:,c) =delta_M_LHC_default delta_x_default(Hneut,c)=delta_Mh_LHC delta_x_default(Hplus,c)=delta_Mhplus_LHC elseif(c.eq.get_collider_element_number('LHC13'))then delta_x_default(:,c) =delta_M_LHC_default delta_x_default(Hneut,c)=delta_Mh_LHC delta_x_default(Hplus,c)=delta_Mhplus_LHC else stop 'error in subroutine setup_S95tables' endif enddo do i=lbound(S95_t1,dim=1),ubound(S95_t1,dim=1) if(S95_t1(i)%deltax.lt.-0.5D0)then !i.e. deltax has not been set yet S95_t1(i)%deltax = delta_x_default(S95_t1(i)%particle_x,WhichColliderElement(S95_t1(i)%expt, S95_t1(i)%energy)) endif enddo do i=lbound(S95_t2,dim=1),ubound(S95_t2,dim=1) if(S95_t2(i)%deltax.lt.-0.5D0)then !i.e. deltax has not been set yet S95_t2(i)%deltax = delta_x_default(S95_t2(i)%particle_x2,WhichColliderElement(S95_t2(i)%expt, S95_t2(i)%energy)) endif enddo ! finds the maximum delta_Mh for the each set of tables ! will be used in theo_SM.f90 to work out which SM para need to be calculated max_expt_delta_Mh= -1.0D0 do i=lbound(S95_t1,dim=1),ubound(S95_t1,dim=1) do c=1,ubound(colliders,dim=1) if(WhichColliderElement(S95_t1(i)%expt, S95_t1(i)%energy).eq.c)then if( S95_t1(i)%particle_x.eq.Hneut)then if(S95_t1(i)%deltax .gt.max_expt_delta_Mh(c))then max_expt_delta_Mh(c)=S95_t1(i)%deltax endif endif endif enddo enddo do i=lbound(S95_t2,dim=1),ubound(S95_t2,dim=1) do c=1,ubound(colliders,dim=1) if(WhichColliderElement(S95_t2(i)%expt, S95_t2(i)%energy).eq.c)then if( S95_t2(i)%particle_x2.eq.Hneut)then !note, this means only cross sections for different particle_x2 will be combined if(S95_t2(i)%deltax .gt.max_expt_delta_Mh(c))then max_expt_delta_Mh(c)=S95_t2(i)%deltax endif endif endif enddo enddo if(debug)write(*,*)'max_expt_delta_Mh',max_expt_delta_Mh ! Exptrange_Mhmin_forSMXS = max(Expttables_Mhmin_forSMXS - max_expt_delta_Mh,0.0D0) ! Exptrange_Mhmax_forSMXS = Expttables_Mhmax_forSMXS + max_expt_delta_Mh ! ! Exptrange_Mhmin_forSMdecays = max(Expttables_Mhmin_forSMdecays - max_expt_delta_Mh,0.0D0) ! Exptrange_Mhmax_forSMdecays = Expttables_Mhmax_forSMdecays + max_expt_delta_Mh Exptrange_Mhmin_forSMXS = max(Expttables_Mhmin_forSMXS,0.0D0) Exptrange_Mhmax_forSMXS = Expttables_Mhmax_forSMXS Exptrange_Mhmin_forSMdecays = max(Expttables_Mhmin_forSMdecays,0.0D0) Exptrange_Mhmax_forSMdecays = Expttables_Mhmax_forSMdecays !we need tevXS_SM_functions to have a big enough range to cover the tables if(Exptrange_Mhmax_forSMXS(get_collider_element_number('TEV ')).gt.tevXS_SM_functions_xmax)then stop 'need to extend upper range of tevXS_SM_functions or reduce delta_M_TEV' endif if(Exptrange_Mhmin_forSMXS(get_collider_element_number('TEV ')).lt.tevXS_SM_functions_xmin)then write(*,*)Exptrange_Mhmin_forSMXS(get_collider_element_number('TEV ')),tevXS_SM_functions_xmin ! TS 24/03/2017: Commented out the following (because some new analyses for low mass Higgses ! do not need these functions (decay from heavier Higgs) ! stop 'need to extend lower range of tevXS_SM_functions' endif !we need lhc7XS_SM_functions to have a big enough range to cover the tables if(Exptrange_Mhmax_forSMXS(get_collider_element_number('LHC7 ')).gt.lhc7XS_SM_functions_xmax)then stop 'need to extend upper range of lhc7XS_SM_functions or reduce delta_M_LHC' endif if(Exptrange_Mhmin_forSMXS(get_collider_element_number('LHC7 ')).lt.lhc7XS_SM_functions_xmin)then ! TS 24/03/2017: Commented out the following (because some new analyses for low mass Higgses ! do not need these functions (decay from heavier Higgs) ! stop 'need to extend lower range of lhc7XS_SM_functions' endif !we need lhc8XS_SM_functions to have a big enough range to cover the tables if(Exptrange_Mhmax_forSMXS(get_collider_element_number('LHC8 ')).gt.lhc8XS_SM_functions_xmax)then stop 'need to extend upper range of lhc8XS_SM_functions or reduce delta_M_LHC' endif if(Exptrange_Mhmin_forSMXS(get_collider_element_number('LHC8 ')).lt.lhc8XS_SM_functions_xmin)then ! write(*,*) Exptrange_Mhmin_forSMXS(get_collider_element_number('LHC8 ')) ! TS 24/03/2017: Commented out the following (because some new analyses for low mass Higgses ! do not need these functions (decay from heavier Higgs) ! stop 'need to extend lower range of lhc8XS_SM_functions' endif !we need lhc8XS_SM_functions to have a big enough range to cover the tables if(Exptrange_Mhmax_forSMXS(get_collider_element_number('LHC13')).gt.lhc13XS_SM_functions_xmax)then stop 'need to extend upper range of lhc13XS_SM_functions or reduce delta_M_LHC' endif if(Exptrange_Mhmin_forSMXS(get_collider_element_number('LHC13')).lt.lhc13XS_SM_functions_xmin)then write(*,*) Exptrange_Mhmin_forSMXS(get_collider_element_number('LHC13')) ! TS 24/03/2017: Commented out the following (because some new analyses for low mass Higgses ! do not need these functions (decay from heavier Higgs) ! stop 'need to extend lower range of lhc13XS_SM_functions' endif ! we need the branching ratios for all the colliders if( maxval(Exptrange_Mhmax_forSMdecays).gt.BRSMt1Mhmax)then ! write(*,*) "hello : ", BRSMt1Mhmax, maxval(Exptrange_Mhmax_forSMdecays) stop 'need to extend upper range of BRfunctions or reduce delta_M_(LEP/TEV)' elseif(minval(Exptrange_Mhmin_forSMdecays).lt.BRSMt1Mhmin)then write(*,*)'hello',minval(Exptrange_Mhmin_forSMdecays),BRSMt1Mhmin stop 'need to extend lower range of BRfunctions' endif deallocate(Expttables_Mhmin_forSMXS) deallocate(Expttables_Mhmax_forSMXS) deallocate(Expttables_Mhmin_forSMdecays) deallocate(Expttables_Mhmax_forSMdecays) deallocate(max_expt_delta_Mh) deallocate(delta_x_default) end subroutine setup_S95tables !********************************************************** function inrange(mass,str) ! mass is the neutral Higgs mass to be checked ! str indicates which range it should be checked against: ! str should be either 'SMBR' or one of the elements of the array 'colliders' ! ! The function returns .True. if the mass is in the appropriate range. ! If str='SMBR', this range is ! minval(Exptrange_Mhmin_forSMdecays) to maxval(Exptrange_Mhmax_forSMdecays) ! otherwise this range is ! Exptrange_Mhmin_forSMXS(x) to Exptrange_Mhmax_forSMXS(x) ! where x is the element of the array 'colliders' character(len=*),intent(in) :: str double precision,intent(in) :: mass logical :: inrange integer :: x, i !-TS(05/07/2012) Added a check whether the ranges are allocated (which happens in !-subroutine setup_S95tables. If not, they are allocated and given default values. !-This is needed for HiggsSignals. if(.not.allocated(Exptrange_Mhmin_forSMXS)) then allocate(Exptrange_Mhmin_forSMXS(size(colliders,dim=1))) allocate(Exptrange_Mhmax_forSMXS(size(colliders,dim=1))) do i=1, size(colliders) if(i.eq.get_collider_element_number('LEP ')) then Exptrange_Mhmin_forSMXS(i)=1.0D0 Exptrange_Mhmax_forSMXS(i)=180.0D0 else if(i.eq.get_collider_element_number('TEV ')) then Exptrange_Mhmin_forSMXS(i)=80.0D0 Exptrange_Mhmax_forSMXS(i)=350.0D0 else if(i.eq.get_collider_element_number('LHC7 ')) then Exptrange_Mhmin_forSMXS(i)=90.0D0 Exptrange_Mhmax_forSMXS(i)=1000.0D0 else if(i.eq.get_collider_element_number('LHC8 ')) then Exptrange_Mhmin_forSMXS(i)=90.0D0 Exptrange_Mhmax_forSMXS(i)=1000.0D0 else if(i.eq.get_collider_element_number('LHC13')) then Exptrange_Mhmin_forSMXS(i)=90.0D0 Exptrange_Mhmax_forSMXS(i)=3000.0D0 else stop 'Error in subroutine inrange. str for XS unknown.' endif enddo endif if(.not.allocated(Exptrange_Mhmin_forSMdecays)) then allocate( Exptrange_Mhmin_forSMdecays(size(colliders,dim=1))) allocate( Exptrange_Mhmax_forSMdecays(size(colliders,dim=1))) do i=1, size(colliders) if(i.eq.get_collider_element_number('LEP ')) then Exptrange_Mhmin_forSMdecays(i)=1.0D0 Exptrange_Mhmax_forSMdecays(i)=180.0D0 else if(i.eq.get_collider_element_number('TEV ')) then Exptrange_Mhmin_forSMdecays(i)=0.2D0 Exptrange_Mhmax_forSMdecays(i)=350.0D0 else if(i.eq.get_collider_element_number('LHC7 ')) then Exptrange_Mhmin_forSMdecays(i)=90.0D0 Exptrange_Mhmax_forSMdecays(i)=1000.0D0 else if(i.eq.get_collider_element_number('LHC8 ')) then Exptrange_Mhmin_forSMdecays(i)=90.0D0 Exptrange_Mhmax_forSMdecays(i)=1000.0D0 else if(i.eq.get_collider_element_number('LHC13')) then Exptrange_Mhmin_forSMdecays(i)=90.0D0 Exptrange_Mhmax_forSMdecays(i)=1000.0D0 else stop 'Error in subroutine inrange. str for decay unknown.' endif enddo endif if(str.eq.'SMBR')then if( (mass.gt.minval(Exptrange_Mhmin_forSMdecays)) & .and.(mass.lt.maxval(Exptrange_Mhmax_forSMdecays)) )then inrange=.True. else inrange=.False. endif else x=get_collider_element_number(str) ! write(*,*) 'debugging inrange:' ! write(*,*) x, mass, Exptrange_Mhmin_forSMXS(x), Exptrange_Mhmax_forSMXS(x) if( (mass.gt.Exptrange_Mhmin_forSMXS(x)) & .and.(mass.lt.Exptrange_Mhmax_forSMXS(x)) )then inrange=.True. else inrange=.False. endif endif end function inrange !********************************************************** function get_collider_element_number(collidername) ! this will return the position of the element with the value 'collidername' in the array 'colliders' !********************************************************** character(len=*),intent(in) :: collidername integer :: x,y integer :: get_collider_element_number y=0 ! print *, collidername do x=lbound(colliders,dim=1),ubound(colliders,dim=1) if(index(colliders(x),collidername).gt.0)then get_collider_element_number=x y=y+1 endif enddo if(y.ne.1)stop 'problem in function get_collider_element_number' end function get_collider_element_number !****************************************************************** function WhichColliderElement(expt,energy) ! this will return the position of the element corresponding to 'expt' in the array 'colliders' !****************************************************************** use usefulbits, only : small character(LEN=3),intent(in) :: expt integer :: WhichColliderElement double precision :: energy if( expt.eq.'LEP' )then WhichColliderElement=get_collider_element_number('LEP ') elseif( (expt.eq.'CDF').or.(expt.eq.' D0').or.(expt.eq.'TCB') )then WhichColliderElement=get_collider_element_number('TEV ') elseif( (expt.eq.'ATL').or.(expt.eq.'CMS') )then if(energy-7.0D0.le.small) then WhichColliderElement=get_collider_element_number('LHC7 ') else if(energy-8.0D0.le.small) then WhichColliderElement=get_collider_element_number('LHC8 ') else if(energy-13.0D0.le.small) then WhichColliderElement=get_collider_element_number('LHC13') else stop 'WhichColliderElement: Collider Energy not correctly specified.' endif else WhichColliderElement=0 endif end function WhichColliderElement !****************************************************************** function WhichColliderString(expt, energy) ! this will return the contents of the element corresponding to 'expt' in the array 'colliders' !****************************************************************** character(LEN=3),intent(in) :: expt character(LEN=5) :: WhichColliderString double precision :: energy ! write(*,*) 'WhichColliderString = ',colliders(WhichColliderElement(expt, energy)) WhichColliderString=colliders(WhichColliderElement(expt, energy)) end function WhichColliderString !****************************************************************** subroutine calcfact(proc,t,cfact,axis_i,axis_j,nc) !****************************************************************** !for table type1, calls calcfact_t1 !for table type2, calls calcfact_t2 !****************************************************************** use usefulbits, only : dataset,listprocesses !internal implicit none !--------------------------------------input type(dataset) :: t type(listprocesses) :: proc !-----------------------------------output double precision :: cfact,axis_j,axis_i integer :: nc !------------------------------------------- select case(proc%ttype) case(1) call calcfact_t1(proc%tlist,proc%findj,t,cfact,axis_i,nc) axis_j=axis_i case(2) call calcfact_t2(proc%tlist,proc%findj,proc%findi,t,cfact,axis_i,axis_j,nc) case default ! ### OS ### cfact = -1D0 return stop 'wrong input to function calcfact in module channels' end select end subroutine calcfact !****************************************************************** subroutine outputproc(proc,k,descrip,specific) !****************************************************************** !for table type1, calls outputproc_t1 !for table type2, calls outputproc_t2 !if neither table applies, writes message !k is where output goes !specific=1 if the specific process should be printed !e.g. ee->h1Z->bbZ !whereas specific==0 if the generic process should be printed !e.g. ee->hiZ->bbZ !****************************************************************** use usefulbits, only : listprocesses !input use likelihoods, only : outputproc_llh implicit none !--------------------------------------input integer,intent(in) :: k,specific integer :: i,j type(listprocesses),intent(in) :: proc character(LEN=200):: descrip !------------------------------------------- select case(specific) case(0) i=0 j=0 case(1) i=proc%findi j=proc%findj case default end select select case(proc%ttype) case(0) descrip='none of the processes apply' case(1) call outputproc_t1(proc%tlist,i,k,descrip) case(2) call outputproc_t2(proc%tlist,i,j,k,descrip) case(9) call outputproc_llh(proc,k,descrip) case default stop 'wrong input to subroutine outputproc in module channels' end select end subroutine outputproc !****************************************************************** subroutine check_against_bound(proc,fact,axis_i,axis_j,ratio,predobs) !****************************************************************** !for table type1, calls interpolate_tabletype1 !for table type2, calls interpolate_tabletype2 !****************************************************************** use usefulbits, only : dataset,listprocesses !internal use interpolate implicit none !--------------------------------------input integer :: predobs double precision :: fact,axis_i,axis_j type(listprocesses) :: proc !-------------------------------------output double precision :: ratio !-----------------------------------internal double precision :: Mi,Mj,interpol !------------------------------------------- interpol=-1.0D0 Mi=axis_i Mj=axis_j if(fact.gt.0.0D0)then select case(proc%ttype) case(1) call interpolate_tabletype1(Mi,S95_t1(proc%tlist),predobs,interpol) case(2) call interpolate_tabletype2(Mi,Mj,S95_t2(proc%tlist),predobs,interpol) case default ! ### OS ### ratio = -1d0 return write(*,*)'wrong input to subroutine check_against_bound in module channels' stop end select endif !--TESTING! ! if(predobs.eq.1) write(*,*) 'Interpolated value = ', interpol if(interpol.ge.0)then ratio=fact/interpol else ratio= -1.0D0 endif end subroutine check_against_bound !********************************************************** subroutine calcfact_t1(c,jj,t,cfact_t1,M_av,nc) !********************************************************** ! calculates fact for table type 1 ! Takes in to account how Standard Model-like parameter point is ! and whether there are any Higgs with slightly higher masses which ! can be combined with his result ! note: numerator and denominator are worked out separately !********************************************************** use usefulbits, only : dataset, np, div, vvsmall, vsmall use theory_BRfunctions use theory_XS_SM_functions implicit none !--------------------------------------input type(dataset) :: t integer :: c,jj !-----------------------------------output double precision :: cfact_t1,M_av integer :: nc !------------------------------------------- integer :: f,j,ii,iii double precision :: M_tot double precision :: BR_Hbb_SM_av,BR_HWW_SM_av,BR_Htautau_SM_av double precision :: tev_XS_HW_SM_av,tev_XS_HZ_SM_av double precision :: tev_XS_H_SM_av double precision :: tev_XS_Hb_SM_av double precision :: tev_XS_ttH_SM_av double precision :: lhc7_XS_H_SM_av double precision :: lhc7_XS_VBF_SM_av double precision :: BR_Zll,BR_Znunu,BR_Wlnu,BR_Ztautau double precision :: BR_Whad,BR_Zhad double precision :: fact_tmp double precision,allocatable :: mass(:),fact(:) integer,allocatable :: model_like(:) integer :: npart !number of particles !source: PDG (Yao et al. J Phys G 33 (2006)) BR_Zll=3.363D-2+3.366D-2 !BR_Zll = sum(l=e,mu), BR(Z ->l+ l-) BR_Znunu=20D-2 !BR_Znunu = BR(Z ->nu_l nu_l-bar) ('invisible') BR_Wlnu=10.75D-2+10.57D-2 !BR_Wlnu = sum(l=e,mu), !BR(W+ ->l+ nu_l) = BR(W- ->l- + nu_l-bar) BR_Whad=67.6D-2 BR_Zhad=69.91D-2 BR_Ztautau=3.370D-2 npart=np( S95_t1(c)%particle_x ) allocate(mass(npart),fact(npart),model_like(npart)) mass(:)=t%particle( S95_t1(c)%particle_x )%M(:) fact= 0.0D0 cfact_t1=0.0D0 model_like=0 !now calculate numerator of 'fact' do j=1,npart if( (abs(mass(jj)-mass(j)).le.S95_t1(c)%deltax) & & .and.( mass(jj).le.mass(j) ) )then select case(S95_t1(c)%id) !these can be compacted, but not doing it yet... doing it at the !same time as revamping the model_likeness test case(142) fact(j)=t%lep%XS_hjZ_ratio(j) *t%BR_hjbb(j) !notice that this is not absolute XS case(143) fact(j)=t%lep%XS_hjZ_ratio(j) *t%BR_hjtautau(j) !notice that this is not absolute XS case(300) fact(j)=t%lep%XS_hjZ_ratio(j) !notice that this is not absolute XS case(400,401,402,403) fact(j)=t%lep%XS_hjZ_ratio(j) *t%BR_hjinvisible(j) !notice that this is not absolute XS case(500) fact(j)=t%lep%XS_hjZ_ratio(j) *t%BR_hjgaga(j) !notice that this is not absolute XS case(600,601) fact(j)=t%lep%XS_hjZ_ratio(j) &!notice that this is not absolute XS & *(t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)) case(711,713) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(721,723,741,743) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(731,733) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(801,811,821) fact(j)=t%lep%XS_HpjHmj_ratio(j)*(t%BR_Hpjcs(j)+t%BR_Hpjcb(j))**2.0D0 !notice that this is not absolute XS case(802) fact(j)=t%lep%XS_HpjHmj_ratio(j)*(t%BR_Hpjcs(j)+t%BR_Hpjcb(j))*2.0D0*t%BR_Hpjtaunu(j) !notice that this is not absolute XS case(803,813) fact(j)=t%lep%XS_HpjHmj_ratio(j)*t%BR_Hpjtaunu(j)**2.0D0 !notice that this is not absolute XS case(8742,4493,9475,5482,5570,5876,1024,9889,3534,6089,10235,3047,10799,3564,6166,6296) fact(j)=t%tev%XS_hjZ_ratio(j) *t%tev%XS_HZ_SM(j) *t%BR_hjbb(j) case(8958,5489,5624,9236,3930,6039,3216,10433,6221,10600) fact(j)=t%tev%XS_hj_ratio(j)*t%tev%XS_H_SM(j) *t%BR_hjWW(j) case(3331) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) fact(j)=fact(j)*t%tev%XS_H_SM(j)*t%BR_HWW_SM(j)!to get the normalisation right case(5757) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(8957,5472,9219,9463,9596,5828,1970,3493,5972,3155,5613,9868,10068,6092,10217,10239,10796,0874,6220) fact(j)=t%tev%XS_hjW_ratio(j) *t%tev%XS_HW_SM(j) *t%BR_hjbb(j) case(5485,7307,5873) fact(j)=t%tev%XS_hjW_ratio(j) *t%tev%XS_HW_SM(j) *t%BR_hjWW(j) case(9071,2491,5740,5980,1014,3363,4555) fact(j)=t%tev%XS_hj_ratio(j) *t%tev%XS_H_SM(j) *t%BR_hjtautau(j) case(8961,0598) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(9284,5503,5726,10105) fact(j)=t%tev%XS_hjb_ratio(j) *t%tev%XS_Hb_SM(j) *t%BR_hjbb(j)/0.9D0/2.0D0 case(6083) fact(j)=t%tev%XS_hjb_ratio(j) *t%tev%XS_Hb_SM(j) *t%BR_hjtautau(j)/0.1D0/2.0D0 case(1514,5601,5737) fact(j)=( t%tev%XS_hjZ_ratio(j) * t%tev%XS_HZ_SM(j) & & + t%tev%XS_hjW_ratio(j) * t%tev%XS_HW_SM(j) & & + t%tev%XS_hj_ratio(j) * t%tev%XS_H_SM(j) & & + t%tev%XS_vbf_ratio(j) * t%tev%XS_vbf_SM(j) & & ) & & * t%BR_hjgaga(j) case(5858,6177,6295,1887,10065,10485,4960) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(7081,9166,9483,5586,9642,1266,0432,9891,5285,3935,6087,6170,10212,6223,6299,10583,10798,10596) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(2012015) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(10010,10607,6436) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(9248,10133,10439) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(4800) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(5845) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(6171) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(9290) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(5984,9714,6006,4481,6095,10432,6179,6302,10599) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(3556,1931) fact(j)=t%tev%XS_hjb_ratio(j) *t%tev%XS_Hb_c2_SM(j) *t%BR_hjbb(j) case(4782) fact(j)=t%tev%XS_hjb_ratio(j) *t%tev%XS_Hb_c1_SM(j) *t%BR_hjbb(j) case(9465,5871,9022,0710,9887,4162,10102,4468) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) !case(9023) ! call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(9674) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(9897,9999) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(0024,5985,0968,5974,4885) fact(j)=t%tev%XS_hjb_ratio(j) *t%tev%XS_Hb_c3_SM(j) *t%BR_hjtautau(j) case(5739,10574) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) fact(j)=fact(j)*t%tev%XS_ttH_SM(j)*t%BR_Hbb_SM(j)!to get the normalisation right case(2012135,12025) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(0611) fact(j)=t%tev%XS_hj_ratio(j)*t%tev%XS_H_SM(j) *t%BR_hjZga(j) case(1269,1270,2011094,13035,160311) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(1811) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(1812,2011138,2011151,2760,2013090,2014050,14020,8353,7712,11002,11008,79152) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(6008,9998) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(6082,6182,6219,6276,10573) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(6096,10606,10806,10884) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(6183,3233) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(6229) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(6286,6301,6304,6305,6309) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(6091,1268) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(2011048,11004,11015,11013,11028,11006,11017,110271,110272,14161,14162,5064,2012017,2011150,2011131) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(2011162,1415,2012092,20130131) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(059301) fact(j)=t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j)*t%BR_hjZZ(j) case(059302) fact(j)=t%lhc8%XS_vbf_ratio(j)*t%lhc8%XS_vbf_SM(j)*t%BR_hjZZ(j) case(20130132) fact(j)=1000.d0*t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j)*t%BR_hjZZ(j)*BR_Zll**2 case(20130133) fact(j)=1000.d0*(t%lhc8%XS_hjZ_ratio(j) * t%lhc8%XS_HZ_SM(j) & & + t%lhc8%XS_hjW_ratio(j) * t%lhc8%XS_HW_SM(j) & & + t%lhc8%XS_vbf_ratio(j) * t%lhc8%XS_vbf_SM(j)) & & * t%BR_hjZZ(j)*BR_Zll**2 case(11025,1997,12041,130021,130022,009361) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) ! write(*,*) "Analysis(130021) fact(",j,")=",fact(j) case(2011026,11005,11016,11026,3478,3357,2011148,2012016) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(110212) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) - case(2011025,2011085,2011161,5895,1414,2012091,2012168,1487,12001,12015,13001,11010,11030,11021) + case(17013,2011025,2011085,2011161,5895,1414,2012091,2012168,1487,12001,12015,13001,11010,11030,11021) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(13006, 13075515,2013009,3051) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(11031,12044,13012) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(13011) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(11034,12039,13009,2012078,12006,12051) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(2011005,3615,2012018,12046) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(2748, 1408, 2012019) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(7214) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(10500) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(11003,11014,2577,11024,1489,12042,13003,13027) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(2011020,2011021) fact(j)=t%lhc7%XS_hj_ratio(j)*t%lhc7%XS_H_SM(j) *t%BR_hjmumu(j) case(5429,2011052,2011111,2011134) fact(j)=t%lhc7%XS_hj_ratio(j)*t%lhc7%XS_H_SM(j) *t%BR_hjWW(j) case(2012012,2012158,2013030) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(10002,5003,2011132,2012094,110201,110292) fact(j)=t%lhc7%XS_hj_ratio(j)*t%lhc7%XS_H_SM(j) *t%BR_hjtautau(j) case(20140492) ! fact(j)=t%lhc8%XS_gg_hj_ratio(j)*t%lhc8%XS_gg_H_SM(j)*t%BR_hjtautau(j) fact(j)=t%lhc8%channelrates(j,6,4)*t%lhc8%XS_gg_H_SM(j) case(2014049) ! fact(j)=t%lhc8%XS_bb_hj_ratio(j)*t%lhc8%XS_bb_H_SM(j)*t%BR_hjtautau(j) fact(j)=t%lhc8%channelrates(j,7,4)*t%lhc8%XS_bb_H_SM(j) case(20160851,160371,20170501) ! fact(j)=t%lhc13%XS_gg_hj_ratio(j)*t%lhc13%XS_gg_H_SM(j)*t%BR_hjtautau(j) ! write(*,*) "debug: ",j,t%lhc13%channelrates(j,6,4) fact(j)=t%lhc13%channelrates(j,6,4)*t%lhc13%XS_gg_H_SM(j) case(20160852,160372,20170502) ! write(*,*) "debug: ",j,t%lhc13%channelrates(j,7,4) ! fact(j)=t%lhc13%XS_bb_hj_ratio(j)*t%lhc13%XS_bb_H_SM(j)*t%BR_hjtautau(j) fact(j)=t%lhc13%channelrates(j,7,4)*t%lhc13%XS_bb_H_SM(j) case(12050,13021) fact(j)=t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j) *t%BR_hjtautau(j) case(11009,11020,2011133,2012014,2012160) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(110291,12043) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(2013010,7663) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(11011,2011163,11022,11032,1488,12008,12045,2011157) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(2011103,2012161,11012) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(13022) fact(j)=t%lhc8%XS_vbf_ratio(j)*div(t%BR_hjWW(j),t%BR_HWW_SM(j) ,0.0D0,1.0D0) case(13013,13441) fact(j)=t%lhc8%XS_vbf_ratio(j)*t%BR_hjinvisible(j) + case(6682) + fact(j)=t%lhc13%XS_vbf_ratio(j)*t%lhc13%XS_vbf_SM(j)*t%BR_hjinvisible(j) case(13018,13442) fact(j)=t%lhc8%XS_hjZ_ratio(j)*t%BR_hjinvisible(j) case(13443) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(2013011,3244) ! Limit is on sigma(HZ)*BR(H->inv)*(BR(Z->ll)+BR(Z->tautau) ! Data given in fb - (multiply by 1000) fact(j)=1000.D0*t%lhc8%XS_hjZ_ratio(j)*t%lhc8%XS_HZ_SM(j) & & *t%BR_hjinvisible(j) !*(BR_Zll+BR_Ztautau) ! print *, 1000.D0*t%lhc8%XS_hjZ_ratio(j)*t%lhc8%XS_HZ_SM(j)*(BR_Zll+BR_Ztautau), fact(j) case(1508329,2015080) fact(j) = t%lhc8%XS_bb_hj_ratio(j)*t%lhc8%XS_bb_H_SM(j)*t%BR_hjbb(j) case(6583) ! Data given in fb - (multiply by 1000) ! (TS 2016/10/13: Added conservatively estimated signal efficiency factor of ~0.56) fact(j)=0.56D0*1000.0D0*( & t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j) + & t%lhc8%XS_vbf_ratio(j)*t%lhc8%XS_vbf_SM(j) + & t%lhc8%XS_hjZ_ratio(j)*t%lhc8%XS_HZ_SM(j) + & t%lhc8%XS_hjW_ratio(j)*t%lhc8%XS_HW_SM(j) + & t%lhc8%XS_tthj_ratio(j)*t%lhc8%XS_ttH_SM(j) ) * t%BR_hjgaga(j) case(14011) do ii=1,npart if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.10.0D0) then fact(j)=fact(j)+1000.0D0 * t%lhc8%XS_hj_ratio(j) * t%lhc8%XS_H_SM(j) & & * t%BR_hjhiZ(j,ii) * BR_Zll * t%BR_hjbb(ii) endif enddo case(17006) ! Data given in fb - (multiply by 1000). ! Limit on leptonic (e,mu,tau) decays of VV -> lnulnu ! BR(W->lnu) = 0.3257 ! BR(Z->ll) = 0.10099 ! BR(Z->nunu) = 0.2000 do ii=1,npart if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.10.0D0) then fact(j)=fact(j)+ 1000.0D0 * t%lhc13%XS_gg_hj_ratio(j) * t%lhc13%XS_gg_H_SM(j) & & * t%BR_hkhjhi(j,ii,ii) * t%BR_hjbb(ii) * & & (t%BR_hjWW(ii) * 0.3257D0**2 + t%BR_hjZZ(ii) * 0.10099D0 * 0.2D0 *2.0D0) endif enddo case(1506534) do ii=1,npart if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.10.0D0) then fact(j)=fact(j)+ t%lhc8%XS_gg_hj_ratio(ii) * t%lhc8%XS_gg_H_SM(ii) & & * t%BR_hkhjhi(ii,j,j) * t%BR_hjtautau(j)**2.0D0 endif enddo case(5051) do ii=1,npart if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.2.5D0) then fact(j)=fact(j)+ t%lhc8%XS_gg_hj_ratio(ii) * t%BR_hkhjhi(ii,j,j)*t%BR_hjgaga(j)**2.0D0 endif enddo case(17020321) do ii=1,npart fact_tmp = 0.0D0 if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.(25.0D0+t%particle(Hneut)%dMh(ii))) then call model_likeness(ii,S95_t1(c)%id,t,model_like(ii),fact_tmp) fact(j) = fact(j) + fact_tmp * t%BR_hkhjhi(ii,j,j) * t%BR_hjtautau(j)**2.0D0 endif enddo - case(17020322) + case(17020322,539) do ii=1,npart ! Multiply by 2.0 because limit is set on BR(H->hh->mumubb) fact_tmp = 0.0D0 if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.(25.0D0+t%particle(Hneut)%dMh(ii))) then call model_likeness(ii,S95_t1(c)%id,t,model_like(ii),fact_tmp) fact(j) = fact(j) + fact_tmp * t%BR_hkhjhi(ii,j,j) * 2.0D0 * t%BR_hjmumu(j) * t%BR_hjbb(j) endif enddo case(17020323) do ii=1,npart ! Multiply by 2.0 because limit is set on BR(H->hh->mumutautau) fact_tmp = 0.0D0 if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.(25.0D0+t%particle(Hneut)%dMh(ii))) then call model_likeness(ii,S95_t1(c)%id,t,model_like(ii),fact_tmp) fact(j) = fact(j) + fact_tmp * t%BR_hkhjhi(ii,j,j) * 2.0D0 * t%BR_hjmumu(j) * t%BR_hjtautau(j) endif enddo case(011812) ! Limit given in fb, multiply by 1000. do ii=1,npart if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.10.0D0) then fact(j)=fact(j)+1000.0D0 * t%lhc8%XS_hj_ratio(j) * t%lhc8%XS_H_SM(j) & & * t%BR_hjhiZ(j,ii) * BR_Zll * t%BR_hjtautau(ii) endif enddo case(011811) ! Limit given in pb do ii=1,npart do iii=1,npart ! No symmetry factor (1/2) because limit is set on BR(H->hh->bbtautau) if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.10.0D0.and.abs(t%particle(Hneut)%M(iii)-125.0D0).lt.10.0D0) then fact(j)=fact(j)+ t%lhc8%XS_hj_ratio(j) * t%lhc8%XS_H_SM(j) & & * t%BR_hkhjhi(j,ii,iii) * ( t%BR_hjtautau(ii) * t%BR_hjbb(iii) + & & t%BR_hjtautau(iii) * t%BR_hjbb(ii) ) endif enddo enddo case(16029) ! Limit given in pb do ii=1,npart do iii=1,npart ! No symmetry factor (1/2) because limit is set on BR(H->hh->bbtautau) if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.10.0D0.and.abs(t%particle(Hneut)%M(iii)-125.0D0).lt.10.0D0) then fact(j)=fact(j)+ t%lhc13%XS_hj_ratio(j) * t%lhc13%XS_H_SM(j) & & * t%BR_hkhjhi(j,ii,iii) * ( t%BR_hjtautau(ii) * t%BR_hjbb(iii) + & & t%BR_hjtautau(iii) * t%BR_hjbb(ii) ) endif enddo enddo case(17002) ! Limit given in fb do ii=1,npart do iii=1,npart ! No symmetry factor (1/2) because limit is set on BR(H->hh->bbtautau) if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.10.0D0.and.abs(t%particle(Hneut)%M(iii)-125.0D0).lt.10.0D0) then fact(j)=fact(j)+ 1000.0D0 * t%lhc13%XS_hj_ratio(j) * t%lhc13%XS_H_SM(j) & & * t%BR_hkhjhi(j,ii,iii) * ( t%BR_hjtautau(ii) * t%BR_hjbb(iii) + & & t%BR_hjtautau(iii) * t%BR_hjbb(ii) ) endif enddo enddo case(2016071) ! Limit given in pb do ii=1,npart do iii=1,npart ! No symmetry factor (1/2) because limit is set on BR(H->hh->WWgaga) if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.2.5D0.and.abs(t%particle(Hneut)%M(iii)-125.0D0).lt.2.5D0) then fact(j)=fact(j)+ t%lhc13%XS_hj_ratio(j) * t%lhc13%XS_H_SM(j) & & * t%BR_hkhjhi(j,ii,iii) * ( t%BR_hjWW(ii) * t%BR_hjgaga(iii) + & & t%BR_hjWW(iii) * t%BR_hjgaga(ii) ) endif enddo enddo case(16002,2016049) ! Limit given in fb, multiply by 1000. do ii=1,npart do iii=1,npart if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.10.0D0.and.abs(t%particle(Hneut)%M(iii)-125.0D0).lt.10.0D0) then fact(j)=fact(j)+ 1000.0D0 * t%lhc13%XS_hj_ratio(j) * t%lhc13%XS_H_SM(j) & & * t%BR_hkhjhi(j,ii,iii) * t%BR_hjbb(iii) * t%BR_hjbb(ii) endif enddo enddo case(14013) ! Limit given in fb, multiply by 1000. do ii=1,npart do iii=1,npart if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.10.0D0.and.abs(t%particle(Hneut)%M(iii)-125.0D0).lt.10.0D0) then fact(j)=fact(j)+ 1000.0D0 * t%lhc8%XS_hj_ratio(j) * t%lhc8%XS_H_SM(j) & & * t%BR_hkhjhi(j,ii,iii) * t%BR_hjbb(iii) * t%BR_hjbb(ii) endif enddo enddo case(044781) ! Limit given in pb (Z->ll unfolded) do ii=1,npart if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.10.0D0) then fact(j)=fact(j) + t%lhc8%XS_gg_hj_ratio(j) * t%lhc8%XS_gg_H_SM(j) & & * t%BR_hjhiZ(j,ii) * t%BR_hjtautau(ii) endif enddo case(044782) ! Limit given in pb (Z->ll unfolded) do ii=1,npart if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.10.0D0) then fact(j)=fact(j) + t%lhc8%XS_gg_hj_ratio(j) * t%lhc8%XS_gg_H_SM(j) & & * t%BR_hjhiZ(j,ii) * t%BR_hjbb(ii) endif enddo case(20160151) ! Limit given in pb (Z->ll unfolded) do ii=1,npart if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.10.0D0) then fact(j)=fact(j) + t%lhc13%XS_gg_hj_ratio(j) * t%lhc13%XS_gg_H_SM(j) & & * t%BR_hjhiZ(j,ii) * t%BR_hjbb(ii) endif enddo case(20160152) ! Limit given in pb (Z->ll unfolded) do ii=1,npart if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.10.0D0) then fact(j)=fact(j) + t%lhc13%XS_bb_hj_ratio(j) * t%lhc13%XS_bb_H_SM(j) & & * t%BR_hjhiZ(j,ii) * t%BR_hjbb(ii) endif enddo case(14006,14037) ! Data given in pb fact(j)= ( & t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j) + & t%lhc8%XS_vbf_ratio(j)*t%lhc8%XS_vbf_SM(j) + & t%lhc8%XS_hjZ_ratio(j)*t%lhc8%XS_HZ_SM(j) + & t%lhc8%XS_hjW_ratio(j)*t%lhc8%XS_HW_SM(j) + & t%lhc8%XS_tthj_ratio(j)*t%lhc8%XS_ttH_SM(j) ) * t%BR_hjgaga(j) + case(2018025) +! Data given in fb (fiducial cross section, multiply here with acceptance functions) + fact(j)= 1000.0D0 * ( & + (0.574D0 - 2.051 * exp(-0.0311*mass(j))) * t%lhc13%XS_hj_ratio(j)*t%lhc13%XS_H_SM(j) + & + (0.663D0 - 1.054 * exp(-0.0182*mass(j))) * t%lhc13%XS_vbf_ratio(j)*t%lhc13%XS_vbf_SM(j) + & + (0.547D0 - 1.223 * exp(-0.0222*mass(j))) * t%lhc13%XS_hjZ_ratio(j)*t%lhc13%XS_HZ_SM(j) + & + (0.547D0 - 1.223 * exp(-0.0222*mass(j))) * t%lhc13%XS_hjW_ratio(j)*t%lhc13%XS_HW_SM(j) + & + (0.663D0 - 1.054 * exp(-0.0182*mass(j))) * t%lhc13%XS_tthj_ratio(j)*t%lhc13%XS_ttH_SM(j) ) * & + t%BR_hjgaga(j) case(14031) fact(j)=1000.0D0* t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j) * & t%BR_hjZga(j)*BR_Zll case(20160821,20160822,063861) fact(j)=t%lhc13%XS_hj_ratio(j)*t%lhc13%XS_H_SM(j)*t%BR_hjZZ(j) case(20160823) fact(j)=t%lhc13%XS_vbf_ratio(j)*t%lhc13%XS_vbf_SM(j)*t%BR_hjZZ(j) case(20160792) ! Data given in fb fact(j)=1000.0D0*t%lhc13%XS_hj_ratio(j)*t%lhc13%XS_H_SM(j)*t%BR_hjZZ(j)*BR_Zll**2 case(20160793) ! Data given in fb fact(j)=1000.0D0*t%lhc13%XS_vbf_ratio(j)*t%lhc13%XS_vbf_SM(j)*t%BR_hjZZ(j)*BR_Zll**2 case(20160741,2016062) fact(j)=t%lhc13%XS_hj_ratio(j)*t%lhc13%XS_H_SM(j)*t%BR_hjWW(j) case(20160742) fact(j)=t%lhc13%XS_vbf_ratio(j)*t%lhc13%XS_vbf_SM(j)*t%BR_hjWW(j) case(2011112) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(2011135) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(6224,6225,6226) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) - case(04670,046701,046702,17030,4873) + case(04670,046701,046702,17030,4873,8567,336) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(0038911,0038912,0038913,0038914) call model_likeness(j,S95_t1(c)%id,t,model_like(j),fact(j)) case(160312,2016088,79151) ! Data given in pb (factor 2 because both signs of the charged Higgs are considered in the limit) fact(j)= 2.0D0 * t%lhc13%XS_Hpjtb(j) * t%BR_Hpjtaunu(j) case(1504233) ! Data given in fb (factor 2 because both signs of the charged Higgs are considered in the limit) fact(j)= 2.0D0 * 1000.0D0*t%lhc8%XS_vbf_Hpj(j) * t%BR_HpjWZ(j) case(2016089) ! Data given in pb (factor 2 because both signs of the charged Higgs are considered in the limit) fact(j)= 2.0D0 * t%lhc13%XS_Hpjtb(j) * t%BR_Hpjtb(j) ! Daniel's attempts case(2016025) fact(j) = t%lhc13%XS_hj_ratio(j) * t%lhc13%XS_H_SM(j) * t%BR_hjbb(j) case(2016044) fact(j) = 1000.0D0*t%lhc13%XS_hj_ratio(j) * t%lhc13%XS_H_SM(j) * t%BR_hjZga(j) case(201608391) do ii=1,npart if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.10.0D0) then fact(j)=fact(j) + t%lhc13%XS_hjW_ratio(ii) *t%lhc13%XS_HW_SM(ii) * t%BR_hkhjhi(ii,j,j) & & * t%BR_hjbb(j) * t%BR_hjbb(j) endif enddo case(16030) fact(j) = t%BR_tHpjb(j) * t%BR_Hpjcs(j) case(2016004) ! Limit given in pb do ii=1,npart do iii=1,npart ! Multiply fact by symmetry factor, 1/2. if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.2.5D0.and.abs(t%particle(Hneut)%M(iii)-125.0D0).lt.2.5D0) then fact(j)=fact(j)+ 0.5D0 * t%lhc13%XS_gg_hj_ratio(j)*t%lhc13%XS_gg_H_SM(j) & & * t%BR_hkhjhi(j,ii,iii) * & & ( t%BR_hjbb(ii)/t%BR_Hbb_SM(ii) * t%BR_hjgaga(iii)/t%BR_Hgaga_SM(iii) + & & t%BR_hjbb(iii)/t%BR_Hbb_SM(iii) * t%BR_hjgaga(ii)/t%BR_Hgaga_SM(ii) ) endif enddo enddo ! case(2016004) ! do ii=1,npart ! if(abs(t%particle(Hneut)%M(ii)-125.0D0).lt.10.0D0.and.t%BR_Hbb_SM(ii).gt.0D0.and.t%BR_Hgaga_SM(ii).gt.0D0) then ! fact(j) + t%lhc13%XS_gg_hj_ratio(j)*t%lhc13%XS_gg_H_SM(j) * t%BR_hkhjhi(j,ii,ii) & ! & * t%BR_hjbb(ii)/t%BR_Hbb_SM(ii) * t%BR_hjgaga(ii)/t%BR_Hgaga_SM(ii) ! endif ! enddo case(1604833) if(abs(t%BR_hjWW(j)/t%BR_hjZZ(j) / (t%BR_HWW_SM(j)/t%BR_HZZ_SM(j))-1.0D0).lt.0.05) then fact(j) = t%lhc13%XS_gg_hj_ratio(j)*t%lhc13%XS_gg_H_SM(j) * (t%BR_hjWW(j) + t%BR_hjZZ(j)) else fact(j) = 0.0D0 endif case(16034) fact(j) = (t%lhc13%XS_hj_ratio(j) * t%lhc13%XS_H_SM(j) + & & t%lhc13%XS_vbf_ratio(j) * t%lhc13%XS_vbf_SM(j) ) * t%BR_hjZZ(j) case(2016056) fact(j) = 1000.0D0*t%lhc13%XS_gg_hj_ratio(j) * t%lhc13%XS_gg_H_SM(j) * t%BR_hjZZ(j) case(15009) fact(j)= 1000.*t%lhc8%XS_bb_hj_ratio(j)*t%lhc8%XS_bb_H_SM(j)*t%BR_hjmumu(j) case(20160551) fact(j) = 1000.0D0*t%lhc13%XS_hj_ratio(j) * t%lhc13%XS_H_SM(j) * t%BR_hjZZ(j) case(20160552) fact(j) = 1000.0D0*t%lhc13%XS_hj_ratio(j) * t%lhc13%XS_H_SM(j) * t%BR_hjWW(j) case default stop 'wrong input to function calcfact_t1 in module S95tables' end select endif enddo if(fact(jj).le.vvsmall)then!A !Higgs jj doesn't contribute - wait until another call of this subroutine before !looking at nearby masses M_av = mass(jj) nc=0 cfact_t1=0.0D0 else!A !find M_av (only using higgs which have non-zero fact): f=0 M_tot=0.0D0 do j=1,npart if( fact(j).gt.vvsmall )then f=f+1 M_tot=M_tot+mass(j) endif enddo nc=f !f will always be > 0 because we've already made sure that fact(jj)>0.0D0 M_av = M_tot/dble(nc) if((WhichColliderString(S95_t1(c)%expt,S95_t1(c)%energy).eq.'LEP'))then!B cfact_t1=sum(fact) elseif(S95_t1(c)%particle_x .ne. Hneut)then!B cfact_t1=sum(fact) else!B ! HB-5 new ---> if(cfact_t1.gt.vvsmall.and.M_av.gt.S95_t1(c)%xmax) then M_av = S95_t1(c)%xmax write(*,*) "WARNING: Evaluating limit of ",trim(adjustl(S95_t1(c)%label))," at upper mass range." else if(cfact_t1.gt.vvsmall.and.M_av.lt.S95_t1(c)%xmin) then M_av = S95_t1(c)%xmin write(*,*) "WARNING: Evaluating limit of ",trim(adjustl(S95_t1(c)%label))," at lower mass range." endif ! <--- if(f.eq.1)then !have already calculated these in theo_manip to save time BR_Hbb_SM_av = t%BR_Hbb_SM(jj) BR_HWW_SM_av = t%BR_HWW_SM(jj) BR_Htautau_SM_av = t%BR_Htautau_SM(jj) tev_XS_HW_SM_av = t%tev%XS_HW_SM(jj) tev_XS_HZ_SM_av = t%tev%XS_HZ_SM(jj) tev_XS_H_SM_av = t%tev%XS_H_SM(jj) tev_XS_Hb_SM_av = t%tev%XS_Hb_SM(jj) tev_XS_ttH_SM_av = t%tev%XS_ttH_SM(jj) lhc7_XS_H_SM_av = t%lhc7%XS_H_SM(jj) lhc7_XS_VBF_SM_av= t%lhc7%XS_vbf_SM(jj) else BR_Hbb_SM_av = BRSM_Hbb(M_av) BR_HWW_SM_av = BRSM_HWW(M_av) BR_Htautau_SM_av = BRSM_Htautau(M_av) tev_XS_HW_SM_av = XS_tev_HW_SM(M_av) tev_XS_HZ_SM_av = XS_tev_HZ_SM(M_av) tev_XS_H_SM_av = XS_tev_gg_H_SM(M_av)+XS_tev_bb_H_SM(M_av) tev_XS_Hb_SM_av = XS_tev_bg_Hb_SM(M_av) tev_XS_ttH_SM_av = XS_tev_ttH_SM(M_av) lhc7_XS_H_SM_av = XS_lhc7_gg_H_SM(M_av)+XS_lhc7_bb_H_SM(M_av) lhc7_XS_VBF_SM_av= XS_lhc7_vbf_SM(M_av) endif ! now include denominator of 'fact' select case(S95_t1(c)%id) case(8742,5482,5570,4493,9475,5876,1024,9889,3534,6089,10235,3047,10799,3564,6166,6296) do j=1,npart fact(j)= div( fact(j) , tev_XS_HZ_SM_av * BR_Hbb_SM_av ,0.0D0,0.0D0) enddo case(8958,5489,5624,9236,3930) do j=1,npart fact(j)= div( fact(j) , tev_XS_H_SM_av * BR_HWW_SM_av ,0.0D0,0.0D0) enddo case(8957,5472,9219,9463,9596,5828,1970,3493,5972,3155,5613,9868,10068,6092,10217,10239,10796,0874,6220) do j=1,npart fact(j)= div( fact(j) , tev_XS_HW_SM_av * BR_Hbb_SM_av ,0.0D0,0.0D0) enddo case(5503,9284,5726,10105) do j=1,npart fact(j)= div( fact(j) , tev_XS_Hb_SM_av ,0.0D0,0.0D0) enddo case(6083) do j=1,npart fact(j)= div( fact(j) , tev_XS_Hb_SM_av ,0.0D0,0.0D0) enddo case(7307,5873) do j=1,npart fact(j)= div( fact(j) , tev_XS_HW_SM_av * BR_HWW_SM_av ,0.0D0,0.0D0) enddo case(8961,0598,10010,9290,9674,9897,9999,10607,6436) case(7081,9166,9483,5586,9642,1266,0432,9891,5285,3935,6087,6170,10212,6223,6299,10583,10798,10596) case(2012015) case(9248,5845,4800,5858,6177,6295,1887,10065,10485,10133,10439,4960) case(9465,5871,9022,9023,0710,9887) case(6171) case(6183,3233) case(6229) case(6304) case(5984,9714,4162,10102,6006,4481,4468,5757,6095,10432,6179,6302,10599) case(5739,10574) do j=1,npart fact(j)= div( fact(j) , tev_XS_ttH_SM_av * BR_Hbb_SM_av ,0.0D0,0.0D0) enddo case(2012135,12025) case(6008,9998) case(6082,6182,6219,6276,10573) case(6096,10606,10806,10884) case(6091,1268) case(5485,9071,2491,5601,1514,3556,5740,4555,0024,5980,1014,5985, & & 0611,3363,6039,3216,0968,5974,1931,4885,6221) case(3331) case(6286,6301,6305,6309) case(10600) case(10433) do j=1,npart fact(j)=div(fact(j) , tev_XS_H_SM_av * BR_HWW_SM_av ,0.0D0,0.0D0) enddo case(2011048,11004,11015,11013,11028,11006,11017,110271,110272,14161,14162,5064,2012017,2011150,2011131) case(2011162,1415,2012092,20130131) case(11025,1997,12041,130021,130022,009361,16034) case(2011026,11005,11016,11026,3478,3357,2011148,2012016) case(110212) - case(2011025,2011085,2011161,5895,1414,2012091,2012168,1487,12001,12015,13001,11010,11030,11021) + case(17013,2011025,2011085,2011161,5895,1414,2012091,2012168,1487,12001,12015,13001,11010,11030,11021) case(13006, 13075515,2013009,3051) case(11031,12044,13012) case(13011) case(11034,12039,13009,2012078,12006,12051) case(2011005,3615,2012018,12046) case(2748, 1408, 2012019) case(7214) case(4782) case(5429,2011052,2011111,2011134) do j=1,npart fact(j)= div( fact(j) , lhc7_XS_H_SM_av * BR_HWW_SM_av ,0.0D0,0.0D0) enddo case(2012012,2012158,2013030) case(10002,5003,2011132,2012094,2014049,20140492,110201,110292,12050,13021) case(059301,059302) case(20130132,20130133) case(11009,11020,2011133,2012014,2012160) case(110291,12043) case(2013010,7663) case(11002,11008) case(11003,11014,2577,11024,1489,12042,13003,13027) case(2011020,2011021) case(10500) case(11011,2011163,11022,11032,1488,12008,12045,2011157) case(2011103,2012161,11012) case(13022) case(13013) - case(13441,13442,13443) + case(13441,13442,13443,6682) case(13018) case(2013011,3244) case(2011112) - case(6583,14006,14037,14031) + case(6583,14006,14037,14031,2018025) case(2011135) case(1508329,2015080) - case(17020321,17020322,17020323) + case(17020321,17020322,17020323,539) case(6224,6225,6226) - case(04670,046701,046702,17030,4873) + case(04670,046701,046702,17030,4873,8567,336) case(0038911,0038912,0038913,0038914) case(160312,2016088,2016089,14011,011811,16029,17002,14013,2016071,16002,011812,20160851,20160852,20170501,20170502,79151) case(1504233,1506534,5051) case(160371,160372,044781,044782,20160151,20160152,17006) case(20160741,20160742,2016062,20160821,20160822,20160823,20160792,20160793,2016049,063861) case(2016025,2016044,201608391,2016004,1604833,2016056,20160551,20160552,15009) case(16030) case default stop 'error calculating denom. in calcfact_t1' end select cfact_t1=sum(fact) endif!B endif!A deallocate(mass) deallocate(fact) deallocate(model_like) end subroutine calcfact_t1 !********************************************************** subroutine calcfact_t2(c,jj,ii,t,cfact_t2,axis_i,axis_j,nc) !********************************************************** !calculates fact for table type 2 !********************************************************** use usefulbits, only : dataset,np,vsmall,not_a_particle,extrapolatewidth implicit none !--------------------------------------input type(dataset) :: t integer :: c,jj,ii !-----------------------------------output double precision :: cfact_t2,axis_i,axis_j integer :: nc !------------------------------------------- integer :: f,i,j,npart2,npart1 double precision :: fact,eps2,crosssection,Mi_av,Mj_av,masstot,BR_Zll,acceptance double precision,allocatable :: massj(:),massi(:) BR_Zll=3.363D-2+3.366D-2 !BR_Zll = sum(l=e,mu), BR(Z ->l+ l-) eps2=0.02D0 npart2=np( S95_t2(c)%particle_x2 ) allocate(massj(npart2)) massj(:)=t%particle( S95_t2(c)%particle_x2 )%M(:) if(S95_t2(c)%particle_x1.eq.not_a_particle)then npart1=1 allocate(massi(npart1)) massi(:)=-1.0D0 else npart1=np( S95_t2(c)%particle_x1 ) allocate(massi(npart1)) massi(:)=t%particle( S95_t2(c)%particle_x1 )%M(:) endif Mj_av=massj(jj) Mi_av=massi(ii) fact= 0.0D0 cfact_t2=0.0D0 masstot=0.0D0 j=jj i=ii f=1 select case(S95_t2(c)%id) case(150) fact=test_appl(t%lep%XS_hjZ_ratio(j)*t%BR_hjhihi(j,i)*t%BR_hjbb(i)**2.0D0)!table 15 hep-ex/0602042 XS ratio case(160) fact=test_appl(t%lep%XS_hjZ_ratio(j)*t%BR_hjhihi(j,i)*t%BR_hjtautau(i)**2.0D0)!table 16 hep-ex/0602042 XS ratio case(180) fact=test_appl(t%lep%XS_hjhi_ratio(j,i)*t%BR_hjbb(j)*t%BR_hjbb(i))!table 18 hep-ex/0602042 XS ratio case(190) fact=test_appl(t%lep%XS_hjhi_ratio(j,i)*t%BR_hjtautau(j)*t%BR_hjtautau(i))!table 19 hep-ex/0602042 XS ratio case(200) fact=test_appl(t%lep%XS_hjhi_ratio(j,i)*t%BR_hjhihi(j,i)*t%BR_hjbb(i)**3.0D0)!table 20 hep-ex/0602042 XS ratio case(210) fact=test_appl(t%lep%XS_hjhi_ratio(j,i)*t%BR_hjhihi(j,i)*t%BR_hjtautau(i)**3.0D0)!table 21 hep-ex/0602042 XS ratio case(220) fact=test_appl(t%lep%XS_hjZ_ratio(j)*t%BR_hjhihi(j,i)*t%BR_hjbb(i)*t%BR_hjtautau(i))!table 22 hep-ex/0602042 XS ratio case(230) fact=test_appl(t%lep%XS_hjhi_ratio(j,i)*t%BR_hjbb(j)*t%BR_hjtautau(i))!table 23 hep-ex/0602042 XS ratio case(240) fact=test_appl(t%lep%XS_hjhi_ratio(j,i)*t%BR_hjtautau(j)*t%BR_hjbb(i))!table 24 hep-ex/0602042 XS ratio case(905) fact=test_appl(t%lep%XS_CpjCmj(j)*t%BR_CjqqNi(j,i)**2.0D0)!fig 5 hep-ex/0401026 absolute XS in fb case(906) fact=test_appl(t%lep%XS_CpjCmj(j)*t%BR_CjqqNi(j,i)*t%BR_CjlnuNi(j,i))!fig 6 hep-ex/0401026 absolute XS in fb case(907) fact=test_appl( t%lep%XS_CpjCmj(j)*t%BR_CjlnuNi(j,i)**2.0D0)!fig 7 hep-ex/0401026 absolute XS in fb case(908) fact=test_appl(t%lep%XS_CpjCmj(j)) !fig 8 hep-ex/0401026 absolute XS in fb case(909) fact=test_appl( t%lep%XS_NjNi(j,i)*t%BR_NjqqNi(j,i)) !fig 9 hep-ex/0401026 absolute XS in fb case(910) fact=test_appl(t%lep%XS_NjNi(j,i))!fig 10 hep-ex/0401026 absolute XS in fb case(6065) fact=test_appl(t%lep%XS_HpjHmj_ratio(j)*(t%BR_Hpjcs(j)+t%BR_Hpjcb(j)+t%BR_Hpjtaunu(j))) case(02671) fact=test_appl(t%lep%XS_HpjHmj_ratio(j)*(t%BR_HpjhiW(j,i)*t%BR_hjbb(i))**2.0D0) case(02672) fact=test_appl( 4.0D0 * t%lep%XS_HpjHmj_ratio(j)*t%BR_HpjhiW(j,i) * & & t%BR_Hpjtaunu(j)*t%BR_hjbb(i)**2.0D0) !Multiplied by 4 (see LEP paper) case(3381) fact=test_appl(t%tev%XS_hj_ratio(j) * t%tev%XS_H_SM(j) * t%BR_hjhihi(j,i) * & & t%BR_hjmumu(i)**2.0D0 )! arXiv:0905.3381 table I, absolute XS in fb case(3382) fact=test_appl(t%tev%XS_hj_ratio(j) * t%tev%XS_H_SM(j) * t%BR_hjhihi(j,i) * & & 2.0D0 * t%BR_hjtautau(i) * t%BR_hjmumu(i) )! arXiv:0905.3381 table II (also using fig 3b), absolute XS in fb case(5053) fact=test_appl(t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j) * t%BR_hjhihi(j,i)) case(13032) ! Limit given in fb, multiply by 1000. fact=test_appl(1000.0D0*t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j)*t%BR_hjhihi(j,i) ) ! case(011811) ! ! Limit given in pb ! fact=test_appl(t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j)*t%BR_hjhihi(j,i) * & ! & t%BR_hjtautau(i) * t%BR_hjbb(i) ) ! case(011812) ! ! Limit given in fb, multiply by 1000. ! fact=test_appl(1000.0D0*t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j)*t%BR_hjhiZ(j,i) * & ! & t%BR_hjtautau(i) * BR_Zll ) ! case(044781) ! ! Limit given in pb (Z->ll unfolded) ! fact=test_appl(t%lhc8%XS_gg_hj_ratio(j)*t%lhc8%XS_gg_H_SM(j)*t%BR_hjhiZ(j,i) * & ! & t%BR_hjtautau(i)) ! case(044782) ! ! Limit given in pb (Z->ll unfolded) ! fact=test_appl(t%lhc8%XS_gg_hj_ratio(j)*t%lhc8%XS_gg_H_SM(j)*t%BR_hjhiZ(j,i) * & ! & t%BR_hjbb(i) ) ! case(20160151) ! ! Limit given in pb (Z->ll unfolded) ! fact=test_appl(t%lhc13%XS_gg_hj_ratio(j)*t%lhc13%XS_gg_H_SM(j)*t%BR_hjhiZ(j,i) * & ! & t%BR_hjbb(i) ) ! case(20160152) ! ! Limit given in pb (Z->ll unfolded) ! fact=test_appl(t%lhc13%XS_bb_hj_ratio(j)*t%lhc13%XS_bb_H_SM(j)*t%BR_hjhiZ(j,i) * & ! & t%BR_hjbb(i) ) case(06896) ! Limit given in fb, multiply by 1000. fact=test_appl(1000.0D0*t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j)*t%BR_hjhihi(j,i) * & & t%BR_hjgaga(i) * t%BR_hjbb(i) ) case(16032) ! Limit given in fb, multiply by 1000. fact=test_appl(1000.0D0*t%lhc13%XS_hj_ratio(j)*t%lhc13%XS_H_SM(j)*t%BR_hjhihi(j,i) * & & t%BR_hjgaga(i) * t%BR_hjbb(i) ) ! case(14013) ! ! Limit given in fb, multiply by 1000. ! fact=test_appl(1000.0D0*t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j)*t%BR_hjhihi(j,i) * & ! & t%BR_hjbb(i) * t%BR_hjbb(i) ) case(16002) ! Limit given in fb, multiply by 1000. fact=test_appl(1000.0D0*t%lhc13%XS_hj_ratio(j)*t%lhc13%XS_H_SM(j)*t%BR_hjhihi(j,i) * & & t%BR_hjbb(i) * t%BR_hjbb(i) ) case(150011) ! Limit given in fb, multiply by 1000. fact=test_appl(1000.0D0*t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j)*t%BR_hjhiZ(j,i) * & & t%BR_hjtautau(i) * BR_Zll ) case(150012) ! Limit given in fb, multiply by 1000. fact=test_appl(1000.0D0*t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j)*t%BR_hjhiZ(j,i) * & & t%BR_hjbb(i) * BR_Zll ) case(16010) ! Limit given in fb, multiply by 1000. fact=test_appl(1000.0D0*t%lhc13%XS_hj_ratio(j)*t%lhc13%XS_H_SM(j)*t%BR_hjhiZ(j,i) * & & t%BR_hjbb(i) * BR_Zll ) case(14022) fact=test_appl( t%BR_hjhihi(j,i) * t%BR_hjtautau(i) * t%BR_hjtautau(i) ) case(150600424) fact=test_appl(1000.0D0*t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j) * & & t%BR_hkhjhi(j,i,i)*t%BR_hjmumu(i)**2.0D0 ) case(16035) fact=test_appl(1000.0D0*t%lhc13%XS_hj_ratio(j)*t%lhc13%XS_H_SM(j) * & & t%BR_hkhjhi(j,i,i)*t%BR_hjmumu(i)**2.0D0 ) case(6227) f=0 do j=1,npart2 if( (abs(massj(jj)-massj(j)).le.S95_t2(c)%deltax) & & .and.( massj(jj).le.massj(j) ) )then crosssection=test_appl( t%tev%XS_hjb_ratio(j)*t%tev%XS_Hb_c4_SM(j) ) if(crosssection.gt.vsmall)then f=f+1 fact=fact+crosssection masstot=massj(j)+masstot endif endif enddo if(f.ne.0)then Mj_av=masstot/dble(f) endif case(02301) fact = ( & t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j) + & t%lhc8%XS_vbf_ratio(j)*t%lhc8%XS_vbf_SM(j) + & t%lhc8%XS_hjZ_ratio(j)*t%lhc8%XS_HZ_SM(j) + & t%lhc8%XS_hjW_ratio(j)*t%lhc8%XS_HW_SM(j) + & t%lhc8%XS_tthj_ratio(j)*t%lhc8%XS_ttH_SM(j) ) * t%BR_hjgaga(j) case(2016059) ! Data given in fb - (multiply by 1000) ! ( Acceptance factor linearly increasing between 200 and 700 GeV, then constant) acceptance = 0.61D0 if(Mj_av.le.700.0D0) then acceptance = ((Mj_av-200.0D0)*0.61D0+(700.0D0-Mj_av)*0.54D0)/500.0D0 endif fact =acceptance*1000.0D0*( & t%lhc13%XS_hj_ratio(j)*t%lhc13%XS_H_SM(j) + & t%lhc13%XS_vbf_ratio(j)*t%lhc13%XS_vbf_SM(j) + & t%lhc13%XS_hjZ_ratio(j)*t%lhc13%XS_HZ_SM(j) + & t%lhc13%XS_hjW_ratio(j)*t%lhc13%XS_HW_SM(j) + & t%lhc13%XS_tthj_ratio(j)*t%lhc13%XS_ttH_SM(j) ) * t%BR_hjgaga(j) case(003892) fact = ( & t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j) + & t%lhc8%XS_vbf_ratio(j)*t%lhc8%XS_vbf_SM(j)) * t%BR_hjWW(j) case(20160791,160331) fact = 1000.0D0 * t%lhc13%XS_hj_ratio(j)*t%lhc13%XS_H_SM(j) * t%BR_hjZZ(j) * BR_Zll**2.0D0 case(160332) fact = 1000.0D0 * t%lhc13%XS_vbf_ratio(j)*t%lhc13%XS_VBF_SM(j) * t%BR_hjZZ(j) * BR_Zll**2.0D0 case(01123) ! Limit given in pb fact = t%lhc13%XS_hj_ratio(j)*t%lhc13%XS_H_SM(j) * t%BR_hjWW(j) case(170121,06386) ! Limit given in pb fact = t%lhc13%XS_hj_ratio(j)*t%lhc13%XS_H_SM(j) * t%BR_hjZZ(j) case default stop 'wrong input to function calcfact_t2 in module S95tables' end select if(S95_t2(c)%particle_x1.eq.not_a_particle)then select case(S95_t2(c)%id) case(6227) axis_i=t%BR_hjtautau(jj) case(02301,2016059,20160791,06386) axis_i=t%particle( S95_t2(c)%particle_x2 )%GammaTot(j) / & & t%particle( S95_t2(c)%particle_x2 )%M(j) case(01123) ! in percent axis_i=t%particle( S95_t2(c)%particle_x2 )%GammaTot(j) / & & t%particle( S95_t2(c)%particle_x2 )%M(j) * 100.0D0 case(003892) axis_i=t%particle( S95_t2(c)%particle_x2 )%GammaTot(j) / & & t%GammaTot_SM(j) case(160331,160332,170121) axis_i=t%particle( S95_t2(c)%particle_x2 )%GammaTot(j) case(6065) axis_i=t%BR_Hpjtaunu(j) case default stop 'Problem in subroutine calcfact_t2 (y1)' end select select case(S95_t2(c)%id) case(02301,2016059,20160791,06386,01123,003892,160331,160332,170121) if(extrapolatewidth) then if(axis_i.gt.S95_t2(c)%xmax1) then axis_i = S95_t2(c)%xmax1 endif endif case default continue end select else axis_i=Mi_av endif if(S95_t2(c)%particle_x2.eq.not_a_particle)then select case(S95_t2(c)%id) case default stop 'Problem in subroutine calcfact_t2 (y2)' end select else axis_j=Mj_av endif cfact_t2=cfact_t2+fact nc=f deallocate(massi) deallocate(massj) contains !******************************************************** function test_appl(x) !******************************************************** use usefulbits, only : div implicit none !--------------------------------------input double precision :: x !-----------------------------------function double precision :: test_appl !------------------------------------------- double precision, allocatable :: XS_ratio(:), ds(:) double precision :: s integer :: k select case(S95_t2(c)%id) case(150,160,180,190,200,210,220,230,240,3381,3382,13032,06896,14013,& & 16002,150011,150012,16032,16029,011811,011812,044781,044782,20160151,& & 20160152,16010,17002,150600424,16035) if(S95_t2(c)%needs_M2_gt_2M1.and.(massj(j).lt.2.0D0*massi(i)))then test_appl=0.0D0 elseif(massj(j).lt.massi(i))then test_appl=0.0D0 else test_appl=x endif case(02671,02672) if(massj(j).lt.massi(i)+3.0D0) then test_appl=0.0D0 else test_appl=x endif case(6065) if( (t%BR_Hpjtaunu(j) + t%BR_Hpjcs(j) + t%BR_Hpjcb(j)).gt.1.0D0 ) then test_appl=0.0D0 write(*,*) 'WARNING: Sum of charged Higgs branching ratios (cs,cb,taunu) > 1.' else test_appl=x endif case(14022) ! SM likeness test of the heavier Higgs boson allocate(XS_ratio(4),ds(4)) XS_ratio=(/ div( t%lhc8%XS_hj_ratio(j),t%lhc8%XS_H_SM(j),0.0D0,1.0D9), & div( t%lhc8%XS_vbf_ratio(j),t%lhc8%XS_vbf_SM(j),0.0D0,1.0D9), & div( t%lhc8%XS_hjW_ratio(j),t%lhc8%XS_HW_SM(j),0.0D0,1.0D9), & div( t%lhc8%XS_hjZ_ratio(j),t%lhc8%XS_HZ_SM(j),0.0D0,1.0D9) /) s=sum(XS_ratio)/4. do k=1,4 ds(k)= div((XS_ratio(k)-s), s, 0.0D0, 1.0D9) enddo if(S95_t2(c)%needs_M2_gt_2M1.and.(massj(j).lt.2.0D0*massi(i)))then test_appl=0.0D0 elseif(massj(j).lt.massi(i))then test_appl=0.0D0 elseif(maxval(ds).gt.0.1D0) then ! SM likeness test of the heavier Higgs boson test_appl=0.0D0 else test_appl=s*x endif case(5053) if(S95_t2(c)%needs_M2_gt_2M1.and.(massj(j).lt.2.0D0*massi(i)))then test_appl=0.0D0 !----Check for sufficiently SM-like BRs to gaga and bb of lighter Higgs elseif(abs(t%BR_hjgaga(i)-t%BR_Hgaga_SM(i)).gt.0.05*t%BR_Hgaga_SM(i)) then test_appl=0.0D0 elseif(abs(t%BR_hjbb(i)-t%BR_Hbb_SM(i)).gt.0.05*t%BR_Hbb_SM(i)) then test_appl=0.0D0 else test_appl=x endif case(905,906,907,909) if(abs(minval(massi)-massi(i)).gt.vsmall)then !checking that lightest neutralino in process is lightest neutralino in model test_appl=0.0D0 elseif(massj(j).lt.massi(i))then test_appl=0.0D0 else test_appl=x endif case(908) if( abs(t%BR_CjWNi(j,i)-1.0D0) .gt. eps2 )then test_appl=0.0D0 elseif(abs(minval(massi)-massi(i)).gt.vsmall)then !checking that lightest neutralino in process is lightest neutralino in model test_appl=0.0D0 elseif(massj(j).lt.massi(i))then test_appl=0.0D0 else test_appl=x endif case(910) if( abs(t%BR_NjZNi(j,i)-1.0D0) .gt. eps2 )then test_appl=0.0D0 elseif(abs(minval(massi)-massi(i)).gt.vsmall)then !checking that lightest neutralino in process is lightest neutralino in model test_appl=0.0D0 elseif(massj(j).lt.massi(i))then test_appl=0.0D0 else test_appl=x endif case(6227) if( ( t%BR_hjtautau(j)+t%BR_hjbb(j) ).le.0.98D0)then test_appl=0.0D0 else test_appl=x endif case default stop 'error in function test_appl' end select end function test_appl end subroutine calcfact_t2 !******************************************************** subroutine outputproc_t1(tlistn,jj,k,descrip) !******************************************************** ! uses information about the process to output a description ! for processes using table type 1 ! note: at the moment, np(x) (and so ii and jj) needs to be 1 digit long i.e. nH<10 !******************************************************** implicit none !--------------------------------------input integer :: tlistn integer :: jj,k !-----------------------------------internal character(LEN=2) :: j character(LEN=45) :: label character(LEN=200):: descrip !------------------------------------------- if(jj.ne.0)then write(j,'(I2)')jj j=adjustl(j) else j='j' endif if(k.eq.21)then label='' !no need to lable each line in Key.dat else label='('//trim(S95_t1(tlistn)%label)//')' endif descrip='' select case(S95_t1(tlistn)%id) case(142) descrip=' (e e)->(h'//j//')Z->(b b-bar)Z ' //label case(143) descrip=' (e e)->(h'//j//')Z->(tau tau)Z ' //label case(300) descrip=' (e e)->(h'//j//')Z->(...)Z ' //label case(400,401,402,403) descrip=' (e e)->(h'//j//')Z->(invisible)Z ' //label case(500) descrip=' (e e)->(h'//j//')Z->(gamma gamma)Z ' //label case(600,601) descrip=' (e e)->(h'//j//')Z->(2 jets)Z ' //label case(711) descrip=' (e e)->b b-bar(h'//j//')->b b-bar(b b-bar) where h'//j//' is CP even ' //label case(713) descrip=' (e e)->b b-bar(h'//j//')->b b-bar(b b-bar) where h'//j//' is CP odd ' //label case(721,741) descrip=' (e e)->b b-bar(h'//j//')->b b-bar(tau tau) where h'//j//' is CP even ' //label case(723,743) descrip=' (e e)->b b-bar(h'//j//')->b b-bar(tau tau) where h'//j//' is CP odd ' //label case(731) descrip=' (e e)->tau tau(h'//j//')->tau tau(tau tau) where h'//j//' is CP even ' //label case(733) descrip=' (e e)->tau tau(h'//j//')->tau tau(tau tau) where h'//j//' is CP odd ' //label case(801,811,821) descrip=' (e e)->(H'//j//'+)(H'//j//'-)->4 quarks ' //label case(802) descrip=' (e e)->(H'//j//'+)(H'//j//'-)->(2 quarks) tau nu ' //label case(803,813) descrip=' (e e)->(H'//j//'+)(H'//j//'-)->tau nu tau nu' //label case(5482,5570,8742,4493,9475,5876,1024,9889,3534,6089,10235,3047,10799,3564,6166,6296) descrip=' (p p-bar)->Z(h'//j//')->l l (b b-bar) ' //label case(9236,3930,8958,6039,3216,10433,6221,10600) descrip=' (p p-bar)->h'//j//'->W W ' //label case(9219,9463,5472,8957,9596,5828,1970,3493,5972,3155,5613,9868,10068,6092,10217,10239,10796,0874,6220,6309) descrip=' (p p-bar)->W(h'//j//')->l nu (b b-bar) ' //label case(5489) descrip=' (p p-bar)->h'//j//'->W W->e mu ' //label case(5624) descrip=' (p p-bar)->h'//j//'->W W->l l ' //label case(3331) descrip=' (p p-bar)->h'//j//'->V V ' //label case(5757) descrip=' (p p-bar)->h'//j//'/VBF->W W->l l where h'//j//' is SM-like ' //label case(5485,5873) descrip=' (p p-bar)->W(h'//j//')->W W W->l l nu nu ' //label case(9071,2491,5740,5980,1014,3363,4555) descrip=' (p p-bar)->h'//j//'->tau tau ' //label case(8961,9465,9290,9713,9674,0598,9897,9998,9999,6008,6096,6183,3233,6229,6304,10606,10806,10884) descrip=' (p p-bar)->h'//j//'+... where h'//j//' is SM-like ' //label case(9284,5503,5726,3556,10105,1931,4782) descrip=' (p p-bar)->h'//j//'(b/b-bar)->(b b-bar) (b/b-bar) ' //label case(6224,6225,6226) descrip=' (p p-bar)->h'//j//'(b/b-bar)->(b b-bar) (b/b-bar) or (tau tau) (b/b-bar) ' //label case(7307) descrip=' (p p-bar)->W(h'//j//')->W W W ' //label case(6301) descrip=' (p p-bar)->V h'//j//'->V W W ' //label case(5601,5737,1514) descrip=' (p p-bar)->h'//j//'+...->gamma gamma+... ' //label case(5858,6177,6295,1887,10065,10485,4960) descrip=' (p p-bar)->h'//j//'+...->gamma gamma+... where h'//j//' is SM-like ' //label case(7081,9166,9483,5586,9642,1266,0432,9891,5285,3935,6087,6170,10212,6223,6299,10583,10798) descrip=' (p p-bar)->V h'//j//'-> (b b-bar) +missing Et where h'//j//' is SM-like ' //label case(10596) descrip=' (p p-bar)->V h'//j//'-> (b b-bar) l nu where h'//j//' is SM-like ' //label case(6091,1268) descrip=' (p p-bar)->V h'//j//'-> ll + X where h'//j//' is SM-like ' //label case(10010) descrip=' (p p-bar)->V (h'//j//')/VBF-> (b b-bar) q q where h'//j//' is SM-like ' //label case(10607) descrip=' (p p-bar)->V (h'//j//')/VBF-> (b b-bar)+... where h'//j//' is SM-like ' //label case(6436) descrip=' (p p-bar)->V (h'//j//')-> (b b-bar)+...' //label case(9248,10133,10439,6305,6286) descrip=' (p p-bar)->h'//j//'+...->tau tau +... where h'//j//' is SM-like ' //label case(4800,5845,6171) descrip=' (p p-bar)->h'//j//'+...->tau tau (2 jets) where h'//j//' is SM-like ' //label case(5871) descrip=' (p p-bar)->h'//j//'+...->W W +... ->l l nu nu +... where h'//j//' is SM-like ' //label case(6082) descrip=' (p p-bar)->h'//j//'+...->V V +... ->e mu missing Et +... where h'//j//' is SM-like ' //label case(6182,6219) descrip=' (p p-bar)->h'//j//'+...->V V +... ->l l missing Et +... where h'//j//' is SM-like ' //label case(6276) descrip=' (p p-bar)->h'//j//'+...->V V +... ->l l l missing Et +... where h'//j//' is SM-like ' //label case(10573) descrip=' (p p-bar)->h'//j//'+...->V V +... ->l l l l +... where h'//j//' is SM-like ' //label case(5984,9714,6006,9022,9023,0710,9887,4162,10102,4481,4468,6095,10432,6179,6302,10599) descrip=' (p p-bar)->h'//j//'+...->W W +... where h'//j//' is SM-like ' //label case(0024,5985,0968,5974,6083,4885) descrip=' (p p-bar)->h'//j//'(b/b-bar)->(tau tau) (b/b-bar) ' //label case(5739,10574) descrip=' (p p-bar)->t t-bar h'//j//'->t t-bar b b-bar ' //label case(2012135,12025) descrip=' (p p)->t t-bar h'//j//'->t t-bar b b-bar ' //label case(0611) descrip=' (p p-bar)->h'//j//'->Z gamma ' //label case(10500) descrip=' (p p-bar)->V h'//j//'-> V tau tau ' //label case(1811) descrip=' t->(H'//j//'+)b->(2 quarks) b ' //label case(1812,2011138,2011151,2760,2013090,2014050,14020,8353,7712,11002,11008,160311,79152) descrip=' t->(H'//j//'+)b->tau nu b ' //label case(1269,1270,2011094,13035) descrip=' t->(H'//j//'+)b->(c s) b' //label case(16030) descrip=' t->(H'//j//'+)b->(c b) b' //label case(11006,11017,110271,110272,14161,14162,5064,2012017,2011150) descrip=' (p p)->h'//j//'/VBF->Z Z-> l l q q where h'//j//' is SM-like ' //label case(2011048,11004,11015,2011131) descrip=' (p p)->h'//j//'/VBF->Z Z-> l l l l where h'//j//' is SM-like ' //label case(2011162,1415,2012092) descrip=' (p p)->h'//j//'/VBF/V h'//j//'->Z Z-> l l l l where h'//j//' is SM-like ' //label case(11025,1997,12041) descrip=' (p p)->h'//j//'/VBF/V/tt h'//j//'->Z Z-> l l l l where h'//j//' is SM-like ' //label case(20130131) descrip=' (p p)->h'//j//'->Z Z-> l l l l where h'//j//' is SM-like ' //label case(20130132) descrip=' (p p)->h'//j//'/ggF h->Z Z-> l l l l ' //label case(20130133) descrip=' (p p)->h'//j//'/VBF/V h->Z Z-> l l l l ' //label case(04670) descrip=' (p p)->h'//j//'->h(SM,125)h(SM,125)-> bb/tautau/WW/gaga (combination) ' //label - case(046701) + case(046701,8567) descrip=' (p p)->h'//j//'->h(SM,125)h(SM,125)-> gaga WW ' //label case(4873) descrip=' (p p)->h'//j//'->h(SM,125)h(SM,125)-> gaga bb ' //label - case(046702) + case(046702,336) descrip=' (p p)->h'//j//'->h(SM,125)h(SM,125)-> bb tautau ' //label case(17030) descrip=' (p p)->h'//j//'->h(SM,125)h(SM,125)-> bb/tautau/WW/ZZ/gaga (combination) ' //label case(059301) descrip=' (p p)->h'//j//'->Z Z ' //label case(059302) descrip=' (p p)->h'//j//'(VBF)->Z Z ' //label case(130021) descrip=' (p p)->h'//j//'->Z Z-> l l l l (low mass) where h'//j//' is SM-like ' //label case(130022) descrip=' (p p)->h'//j//'->Z Z-> l l l l (high mass) where h'//j//' is SM-like ' //label case(16034) descrip=' (p p)->h'//j//'/VBF->Z Z-> l l q q, with single-Higgs/VBF ratio profiled ' //label case(009361) descrip=' (p p)->h'//j//'->V V where h'//j//' is SM-like ' //label case(11005,11016,11026,3478) descrip=' (p p)->h'//j//'/VBF->V V-> l l nu nu where h'//j//' is SM-like ' //label case(3357,2011148,2012016) descrip=' (p p)->h'//j//'->V V-> l l nu nu where h'//j//' is SM-like ' //label case(11013,11028) descrip=' (p p)->h'//j//'/VBF->V V-> l l tau tau where h'//j//' is SM-like ' //label case(2011026) descrip=' (p p)->h'//j//'/VBF->V V where h'//j//' is SM-like ' //label case(5429,2011052,2011111,2011134) descrip=' (p p)->h'//j//'->W W ' //label case(063861) descrip=' (g g)->h'//j//' -> Z Z -> 4l+2l2nu (employs NWA)' //label case(20160821) descrip=' (g g)->h'//j//' -> Z Z -> llnunu (employs NWA)' //label case(20160822) descrip=' (g g)->h'//j//' -> Z Z -> llqq (employs NWA)' //label case(20160792) descrip=' (g g)->h'//j//' -> Z Z -> 4l (low-mass range, employs NWA)' //label case(20160823) descrip=' (p p)->h'//j//'(VBF) -> Z Z -> llqq (employs NWA)' //label case(2016062) descrip=' (p p)->h'//j//' -> W W -> lnuqq (employs NWA)' //label case(20160741) descrip=' (p p)->h'//j//' -> W W -> lnulnu (employs NWA)' //label case(20160742) descrip=' (p p)->h'//j//'(VBF) -> W W -> lnulnu (employs NWA)' //label case(20160793) descrip=' (p p)->h'//j//'(VBF) -> Z Z -> 4l (employs NWA)' //label case(0038911) descrip=' (p p)->h'//j//'->W W (employs NWA)' //label case(0038912) descrip=' (p p)->VBF, h'//j//'->W W (employs NWA)' //label case(0038913) descrip=' (p p)->h'//j//'->W W (assumes SM Higgs width, employs CPS)' //label case(0038914) descrip=' (p p)->VBF, h'//j//'->W W (assumes SM Higgs width, employs CPS)' //label case(11034,12039,13009,2012078) descrip=' (p p)->W(h'//j//')->W W W where h'//j//' is SM-like ' //label case(12006) descrip=' (p p)->W(h'//j//')->W tau tau ' //label case(12051) descrip=' (p p)->V(h'//j//')->V tau tau ' //label case(2012012,2012158,2013030) descrip=' (p p)->h'//j//'->W W where h'//j//' is SM-like ' //label case(110212) descrip=' (p p)->V h'//j//'/VBF->gamma gamma ' //label - case(2011025,2011085,2011161,5895,1414,2012091,2012168,1487,12001,12015,13001,11010,11030,11021) + case(17013,2011025,2011085,2011161,5895,1414,2012091,2012168,1487,12001,12015,13001,11010,11030,11021) descrip=' (p p)->h'//j//'+...->gamma gamma+... where h'//j//' is SM-like ' //label - case(6583,14006,14037) + case(6583,14006,14037,2018025) descrip=' (p p)->h'//j//'/VBF/Wh'//j//'/Zh'//j//'/tth'//j//'->gamma gamma ' //label case(14031) descrip=' (p p)->h'//j//'->Z gamma -> l l gamma ' //label case(13006, 13075515,2013009,3051) descrip=' (p p)->h'//j//'+...->gamma Z+... where h'//j//' is SM-like ' //label case(11031,12044,13012) descrip=' (p p)->V h'//j//'->b b where h'//j//' is SM-like ' //label case(13011) descrip=' (p p)->h'//j//'/VBF->bb+... where h'//j//' is SM-like ' //label case(2011020,2011021) descrip=' (p p)->h'//j//'->mu mu (lower mass range) ' //label case(2011005,3615,2012018) descrip=' (p p)->h'//j//'/VBF->W W where h'//j//' is SM-like ' //label case(12046) descrip=' (p p)->h'//j//'->W W-> l nu q q where h'//j//' is SM-like ' //label case(11003,11014,2577,11024,1489,12042,13003,13027) descrip=' (p p)->h'//j//'+...->W W +... where h'//j//' is SM-like ' //label case(2748,1408,11011,2011163,11022,11032,1488,12008,12045,2011157,2011112,2011135,2012019) descrip=' (p p)->h'//j//'+... where h'//j//' is SM-like ' //label case(7214) descrip=' (p p)->h'//j//'+... where h'//j//' is SM-like ' //label case(10002,5003,2011132,2012094,110201,110292,12050,13021) descrip=' (p p)->h'//j//'->tau tau ' //label case(2014049,20160852,160372,20170502) descrip=' (p p)->bbh'//j//'->tau tau ' //label case(20140492,20160851,160371,20170501) descrip=' (p p)->ggh'//j//'->tau tau ' //label case(11009,11020,2011133,2012014) descrip=' (p p)->h'//j//'/VBF->tau tau +... where h'//j//' is SM-like ' //label case(2012160,12043) descrip=' (p p)->h'//j//'->tau tau +... where h'//j//' is SM-like ' //label case(2013010,7663) descrip=' (p p)->h'//j//'->mu mu +... where h'//j//' is SM-like ' //label case(2012015) descrip=' (p p)->V h'//j//'-> (b b-bar) + X where h'//j//' is SM-like ' //label case(110291) descrip=' (p p)->h'//j//'/VBF/V h'//j//'/tt h'//j//'->tau tau +... where h'//j//' is SM-like ' //label case(2011103,2012161,11012) descrip=' (p p)->V(h'//j//')->V (b b-bar) ' //label case(13022) descrip=' (p p)->h'//j//'(VBF)->WW ' //label - case(13013,13441) + case(13013,13441,6682) descrip=' (p p)->h'//j//'(VBF)->V (invisible) ' //label case(13018,13442) descrip=' (p p)->Zh'//j//'->Z (invisible) ' //label case(13443) descrip=' (p p)->h'//j//'(VBF)/Zh'//j//', h'//j//'->(invisible) ' //label case(2013011,3244) descrip=' (p p)->Vh'//j//'->V (invisible) ' //label case(160312,2016088,79151) descrip=' (p p) -> (H'//j//'+) t b -> (tau nu) t b '//label case(1504233) descrip=' (p p) -> (H'//j//'+) (VBF) -> W Z '//label case(2016089) descrip=' (p p) -> (H'//j//'+) t b -> (t b) t b '//label case(2016071) descrip=' (p p) -> h'//j//' -> h h -> W W gamma gamma, where h lies around 125 (+- 2.5 GeV) '//label case(14013,16002,2016049) descrip=' (p p) -> h'//j//' -> h h -> b b b b, where h lies around 125 (+- 10 GeV) '//label case(011811,16029,17002) descrip=' (p p) -> h'//j//' -> h h -> b b tau tau, where h lies around 125 (+- 10 GeV) '//label case(14011,044782) descrip=' (p p) -> h'//j//' -> Z h -> l l b b, where h lies around 125 (+- 10 GeV) '//label case(011812,044781) descrip=' (p p) -> h'//j//' -> Z h -> l l tau tau, where h lies around 125 (+- 10 GeV) '//label case(20160151) descrip=' (g g) -> h'//j//' -> Z h -> l l b b, where h lies around 125 (+- 10 GeV) '//label case(20160152) descrip=' (b b) -> h'//j//' -> Z h -> l l b b, where h lies around 125 (+- 10 GeV) '//label case(1508329,2015080) descrip=' (p p)->bbh'//j//'->b b ' //label case(2016025) descrip=' (p p)->h'//j//'->b b ' //label case(2016044) descrip=' (p p)->h'//j//'->Z gamma ' //label case(201608391) descrip=' (p p) -> W h -> W a a -> W b b b b, where h lies around 125 (+- 10 GeV) '//label case(15009) descrip=' (p p)->b b h'//j//'->b b mu mu ' //label case(2016004) descrip=' (p p)->h'//j//'->h h -> b b gamma gamma, where h lies around 125 (+- 2.5 GeV) ' //label case(17006) descrip=' (p p)->h'//j//'->h h -> b b l l nu nu, where h lies around 125 (+- 10 GeV) ' //label case(1604833) descrip=' (p p)->h'//j//'->V V (V=W,Z) ' //label case(2016056) descrip=' (p p)->h'//j//'->Z Z-> l l nu nu ' //label case(20160551) descrip=' (p p)->h'//j//'->Z Z-> q q q q (boosted jets, using RS graviton limit) ' //label case(20160552) descrip=' (p p)->h'//j//'->W W-> q q q q (boosted jets, using RS graviton limit) ' //label case(17020321,1506534) descrip=' (p p)-> H_{SM-like} near 125 GeV -> h'//j//'h'//j//' -> tau tau tau tau ' //label case(5051) descrip=' (p p)-> H_{SM-like} near 125 GeV -> h'//j//'h'//j//' -> gamma gamma gamma gamma ' //label - case(17020322) + case(17020322,539) descrip=' (p p)-> H_{SM-like} near 125 GeV -> h'//j//'h'//j//' -> mu mu b b ' //label case(17020323) descrip=' (p p)-> H_{SM-like} near 125 GeV -> h'//j//'h'//j//' -> mu mu tau tau ' //label case default stop 'wrong input to function outputproc_t1 in module S95tables (1)' end select ! New description string based on data file input ! Added by OS 2012-03-12 if(S95_t1(tlistn)%desc.NE.'') then descrip = trim(S95_t1(tlistn)%desc) // ', h='//j if (S95_t1(tlistn)%SMlike.EQ.1) then descrip = trim(descrip)//' where h is SM-like' endif descrip = trim(descrip)//' '//label endif end subroutine outputproc_t1 !******************************************************** subroutine outputproc_t2(tlistn,ii,jj,k,descrip) !******************************************************** ! uses information about the process to output a description ! for processes using table type 1 ! note: at the moment, np(x) (and so ii and jj) needs to be 1 digit long i.e. np(x)<10 !******************************************************** implicit none !--------------------------------------input integer :: tlistn integer :: ii,jj,k !-----------------------------------internal character(LEN=2) :: j,i character(LEN=45) :: label character(LEN=200):: descrip !------------------------------------------- if((ii.ne.0).and.(jj.ne.0))then write(i,'(I2)')ii i=adjustl(i) write(j,'(I2)')jj j=adjustl(j) else i='i' j='j' endif if(k.eq.21)then label='' !no need to lable each line in Key.dat else label='('//trim(S95_t2(tlistn)%label)//')' endif select case(S95_t2(tlistn)%id) case(150) descrip=' (ee)->(h'//j//'->h'//i//' h'//i//')Z->(b b b b)Z ' //label case(160) descrip=' (ee)->(h'//j//'->h'//i//' h'//i//')Z->(tau tau tau tau)Z ' //label case(180) descrip=' (ee)->(h'//j//' h'//i//')->(b b b b) ' //label case(190) descrip=' (ee)->(h'//j//' h'//i//')->(tau tau tau tau) ' //label case(200) descrip=' (ee)->(h'//j//'->h'//i//' h'//i//')h'//i//'->(b b b b)b b '//label case(210) descrip=' (ee)->(h'//j//'->h'//i//' h'//i//')h'//i//'->(tau tau tau tau)tau tau '//label case(220) descrip=' (ee)->(h'//j//'->h'//i//' h'//i//')Z->(b b)(tau tau)Z ' //label case(230) descrip=' (ee)->(h'//j//'->b b)(h'//i//'->tau tau) ' //label case(240) descrip=' (ee)->(h'//j//'->tau tau)(h'//i//'->b b) ' //label case(905) descrip=' (ee)->(C'//j//'+)(C'//j//'-)-> (q q N'//i//') (q q N'//i//') ' //label case(906) descrip=' (ee)->(C'//j//'+)(C'//j//'-)-> q q l nu N'//i//' N'//i//' ' //label case(907) descrip=' (ee)->(C'//j//'+)(C'//j//'-)-> (l nu N'//i//') (l nu N'//i//') ' //label case(908) descrip=' (ee)->(C'//j//'+)(C'//j//'-) with all C'//j//' decaying to W + N'//i//' ' //label case(909) descrip=' (ee)->(N'//j//') N'//i//'-> (q q N'//i//') N'//i//' ' //label case(910) descrip=' (ee)->N'//j//' N'//i//' with all N'//j//' decaying to Z + N'//i//' ' //label case(6065) descrip=' (ee)->(H'//j//'+)(H'//j//'-), with H^(+/-) -> 2 quarks or tau nu (combination)' //label case(02671) descrip=' (ee)->(H'//j//'+)(H'//j//'-)-> (h'//i//'W)(h'//i//'W), with h'//i//'-> bb' //label case(02672) descrip=' (ee)->(H'//j//'+)(H'//j//'-)-> (h'//i//'W)(tau nu), with h'//i//'-> bb' //label case(3381) descrip=' (p p-bar)->h'//j//'->h'//i//' h'//i//'->mu mu mu mu ' //label case(3382) descrip=' (p p-bar)->h'//j//'->h'//i//' h'//i//'->tau tau mu mu ' //label case(5053) descrip=' (p p)->h'//j//'->h'//i//' h'//i//'->gamma gamma b b, where h'//i//' is SM-like around 125 GeV '//label case(13032,06896,16032) descrip=' (p p)->h'//j//'->h'//i//' h'//i//'->gamma gamma b b, where h'//i//' lies around 125 GeV '//label case(011811) descrip=' (p p)->h'//j//'->h'//i//' h'//i//'->b b tau tau, where h'//i//' lies around 125 GeV '//label case(14013,16002) descrip=' (p p)->h'//j//'->h'//i//' h'//i//'->b b b b, where h'//i//' lies around 125 GeV '//label case(14022) descrip=' (p p)->h'//j//'->h'//i//' h'//i//'->tau tau tau tau, where h'//j//' lies around 125 GeV and is SM-like '//label case(011812,150011) descrip=' (p p)->h'//j//' -> h'//i//'Z -> (tau tau)(l l) '//label case(150012,16010) descrip=' (p p)->h'//j//' -> h'//i//'Z -> (b b-bar)(l l) '//label case(044781) descrip=' (g g)->h'//j//' -> h'//i//'Z -> (tau tau)(l l) '//label case(044782,20160151) descrip=' (g g)->h'//j//' -> h'//i//'Z -> (b b-bar)(l l) '//label case(20160152) descrip=' (b b)->h'//j//' -> h'//i//'Z -> (b b-bar)(l l) '//label case(6227) descrip=' (p p-bar)->h'//j//'(b/b-bar)->(b b-bar) (b/b-bar) or (tau tau) (b/b-bar) ' //label case(02301,2016059) descrip=' (p p)->h'//j//'/VBF/Wh'//j//'/Zh'//j//'/tth'//j//'->gamma gamma (including widths effects) ' //label case(003892) descrip=' (p p)->h'//j//'/VBF->W W (including widths effects) ' //label case(01123) descrip=' (p p)->h'//j//'->W W (including widths effects) ' //label case(20160791,160331) descrip=' (g g)->h'//j//'->Z Z -> 4l (including widths effects) ' //label case(170121) descrip=' (p p)->h'//j//'->Z Z -> 4l,2l2q,2l2nu (including widths effects) ' //label case(06386) descrip=' (p p)->h'//j//'->Z Z -> 4l,2l2nu (including widths effects) ' //label case(160332) descrip=' (p p)->h'//j//' (VBF)->Z Z -> 4l (including widths effects) ' //label case(150600424,16035) descrip=' (p p)->h'//j//'->h'//i//'h'//i//'->mu mu mu mu ' //label case default stop 'wrong input to function outputproc_t2 in module S95tables (2)' end select end subroutine outputproc_t2 !****************************************************************** subroutine model_likeness(j,id,t,model_like,sigmaXbr) !***************************************************************** ! Tests how Standard Model-like a parameter point is ! 0 means Mi.ge.MSingleLim (treat as single channel) ! 1 passes the SM-like test and Mi.lt.MSingleLim ! -1 fails the SM-like test and Mi.lt.MSingleLim use usefulbits, only : dataset,div, vsmall, iselementofarray, np, Hneut use theory_BRfunctions use theory_XS_SM_functions implicit none !--------------------------------------input type(dataset) :: t integer :: id,j !-----------------------------------internal integer :: ns,nb,n,jj !--TS 14/03/2011: For revamped model-likeness test method double precision,allocatable :: channel_rat(:,:), channel_SM(:,:) double precision,allocatable :: XS_SM_temp(:), BR_SM_temp(:) double precision :: SMrate, weight, c, dcbyc_dble integer :: ic,nc,nc_rel !---- double precision,allocatable :: XS_rat(:), BR_rat(:) integer :: model_like,testSMratios double precision :: sigmaXbr integer :: is,ib double precision :: s,b double precision,allocatable :: dsbys(:),dbbyb(:),dcbyc(:) logical :: correct_properties double precision,parameter :: unset=-9.9999D6 correct_properties=.True. ns=-1 nb=-1 nc=-1 n=t1elementnumberfromid(S95_t1,id) select case(id) case(711,713,721,723,731,733,741,743,5739,10574,6224,6225,6226,6276,6301,6309,& - & 04670,046701,046702,0038911,0038912,0038913,0038914,17030,4873) + & 04670,046701,046702,336,0038911,0038912,0038913,0038914,17030,4873,8567) !these have a very simple model-likeness test, so we can have a non-zero deltax case default if(S95_t1(n)%deltax.gt.0.0D0)then write(*,*)'hello id=',id,'deltax=',S95_t1(n)%deltax stop 'error in subroutine model_likeness (1)' endif end select select case(id) case(8961,0598) ! ns = 3; nb = 2; call initialise_XS_rat_BR_rat nc = 6; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hj_ratio(j) ! XS_rat(3) = t%tev%XS_hjZ_ratio(j) ! BR_rat(1) = div(t%BR_hjbb(j) , t%BR_Hbb_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div(t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(5,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(6,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hbb_SM(j) /) case(10010,10607) ! ns = 4; nb = 2; call initialise_XS_rat_BR_rat nc = 8; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_vbf_ratio(j) ! XS_rat(3) = t%tev%XS_hjZ_ratio(j) ! XS_rat(4) = t%tev%XS_tthj_ratio(j) ! BR_rat(1) = div(t%BR_hjbb(j) , t%BR_Hbb_SM(j),0.0D0,1.0D0) ! BR_rat(2) = div(( t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j) ) & ! & , t%BR_Hjets_SM(j),0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(5,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(6,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(7,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(8,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hbb_SM(j) /) case(13443) nc = 2; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc8%XS_hjZ_ratio(j) , div(t%BR_hjinvisible(j),1.0D0,0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc8%XS_vbf_ratio(j) , div(t%BR_hjinvisible(j),1.0D0,0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc8%XS_HZ_SM(j) , 1.0D0 /) channel_SM(2,:) = (/ t%lhc8%XS_vbf_SM(j) , 1.0D0 /) case(6436) nc = 2; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hbb_SM(j) /) case(9290) ! ns = 4; nb = 4; call initialise_XS_rat_BR_rat nc = 16; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hj_ratio(j) ! XS_rat(3) = t%tev%XS_hjZ_ratio(j) ! XS_rat(4) = t%tev%XS_vbf_ratio(j) ! BR_rat(1) = div( t%BR_hjbb(j) , t%BR_Hbb_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(3) = div(t%BR_hjtautau(j) , t%BR_Htautau_SM(j),0.0D0,1.0D0) ! BR_rat(4) = div( t%BR_hjgaga(j) , t%BR_Hgaga_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(11,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(12,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(13,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(14,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(15,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(16,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%tev%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(6,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(7,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(8,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(9,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(10,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(11,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(12,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(13,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(14,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(15,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(16,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hgaga_SM(j) /) case(9674,9897,9999) ! ns = 4; nb = 3; call initialise_XS_rat_BR_rat nc = 12; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hj_ratio(j) ! XS_rat(3) = t%tev%XS_hjZ_ratio(j) ! XS_rat(4) = t%tev%XS_vbf_ratio(j) ! BR_rat(1) = div( t%BR_hjbb(j) , t%BR_Hbb_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(3) = div(t%BR_hjtautau(j) , t%BR_Htautau_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(11,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(12,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%tev%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(6,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(7,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(8,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(9,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(10,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(11,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(12,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hbb_SM(j) /) case(7081,9166,9483,5586,9642,1266,0432,9891,5285,3935,6087,6170,10212,6223,6299,10583,10798,10596) ! ns = 2; nb = 1; call initialise_XS_rat_BR_rat nc = 2; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hjZ_ratio(j) ! BR_rat(1) = div(t%BR_hjbb(j) , t%BR_Hbb_SM(j),0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hbb_SM(j) /) case(10500) ! ns = 2; nb = 1; call initialise_XS_rat_BR_rat nc = 2; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hjZ_ratio(j) ! BR_rat(1) = div(t%BR_hjtautau(j) , t%BR_Htautau_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Htautau_SM(j) /) case(9248,10133,10439) ! ns = 4; nb = 1; call initialise_XS_rat_BR_rat nc = 4; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hj_ratio(j) ! XS_rat(3) = t%tev%XS_hjZ_ratio(j) ! XS_rat(4) = t%tev%XS_vbf_ratio(j) ! BR_rat(1) = div(t%BR_hjtautau(j) , t%BR_Htautau_SM(j),0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Htautau_SM(j) /) case(4800) ! ns = 4; nb = 3; call initialise_XS_rat_BR_rat nc = 12; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hj_ratio(j) ! XS_rat(3) = t%tev%XS_hjZ_ratio(j) ! XS_rat(4) = t%tev%XS_vbf_ratio(j) ! BR_rat(1) = div(t%BR_hjtautau(j) , t%BR_Htautau_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div(t%BR_hjbb(j) , t%BR_Hbb_SM(j),0.0D0,1.0D0) ! BR_rat(3) = div(( t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j) ) & ! & , t%BR_Hjets_SM(j),0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%tev%XS_hj_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%tev%XS_vbf_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%tev%XS_hjW_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%tev%XS_hjZ_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(11,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(12,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(5,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(6,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(7,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(8,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(9,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(10,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(11,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(12,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hbb_SM(j) /) case(5845) ! ns = 4; nb = 2; call initialise_XS_rat_BR_rat nc = 8; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hj_ratio(j) ! XS_rat(3) = t%tev%XS_hjZ_ratio(j) ! XS_rat(4) = t%tev%XS_vbf_ratio(j) ! BR_rat(1) = div(t%BR_hjtautau(j) , t%BR_Htautau_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div(( t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j) ) & ! & , t%BR_Hjets_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%tev%XS_hj_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%tev%XS_vbf_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%tev%XS_hjW_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%tev%XS_hjZ_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(5,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(6,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(7,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(8,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hjets_SM(j) /) case(5858,6177,6295,1887,10065,10485,4960) ! ns = 4; nb = 1; call initialise_XS_rat_BR_rat nc = 4; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hj_ratio(j) ! XS_rat(3) = t%tev%XS_hjZ_ratio(j) ! XS_rat(4) = t%tev%XS_vbf_ratio(j) ! BR_rat(1) = div(t%BR_hjgaga(j) , t%BR_Hgaga_SM(j),0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hgaga_SM(j) /) case(9465,5871,9022,9023,0710,9887,5984,9714,4162,10102,6006,4481,4468,6095,10432,6179,6302,10599) ! ns = 4; nb = 1; call initialise_XS_rat_BR_rat nc = 4; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hj_ratio(j) ! XS_rat(3) = t%tev%XS_hjZ_ratio(j) ! XS_rat(4) = t%tev%XS_vbf_ratio(j) ! BR_rat(1) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HWW_SM(j) /) case(6082,6182,6219,10573,6276) ! ns = 4; nb = 2; call initialise_XS_rat_BR_rat nc = 8; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hj_ratio(j) ! XS_rat(3) = t%tev%XS_hjZ_ratio(j) ! XS_rat(4) = t%tev%XS_vbf_ratio(j) ! BR_rat(1) = div(t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div(t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%tev%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(6,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(7,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(8,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HZZ_SM(j) /) case(3331) ! ns = 1; nb = 2; call initialise_XS_rat_BR_rat nc = 2; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hj_ratio(j) ! BR_rat(1) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div( t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_H_SM(j) , t%BR_HZZ_SM(j) /) case(6301) ! ns = 2; nb = 1; call initialise_XS_rat_BR_rat nc = 2; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hjZ_ratio(j) ! BR_rat(1) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HWW_SM(j) /) case(6309) ! ns = 4; nb = 2; call initialise_XS_rat_BR_rat nc = 5; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HWW_SM(j) /) case(1268,6091) ! ns = 2; nb = 2; call initialise_XS_rat_BR_rat nc = 4; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hjZ_ratio(j) ! BR_rat(1) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div( t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HZZ_SM(j) /) case(6008,9998) ! ns = 5; nb = 5; call initialise_XS_rat_BR_rat nc = 25; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hj_ratio(j) ! XS_rat(3) = t%tev%XS_hjZ_ratio(j) ! XS_rat(4) = t%tev%XS_vbf_ratio(j) ! XS_rat(5) = t%tev%XS_tthj_ratio(j) ! BR_rat(1) = div( t%BR_hjbb(j) , t%BR_Hbb_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(3) = div(t%BR_hjtautau(j) , t%BR_Htautau_SM(j) ,0.0D0,1.0D0) ! BR_rat(4) = div(t%BR_hjgaga(j) , t%BR_Hgaga_SM(j) ,0.0D0,1.0D0) ! BR_rat(5) = div(( t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j) ) & ! & , t%BR_Hjets_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%tev%XS_tthj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%tev%XS_tthj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(11,:) = (/ t%tev%XS_hj_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(12,:) = (/ t%tev%XS_vbf_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(13,:) = (/ t%tev%XS_hjW_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(14,:) = (/ t%tev%XS_hjZ_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(15,:) = (/ t%tev%XS_tthj_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(16,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(17,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(18,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(19,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(20,:) = (/ t%tev%XS_tthj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(21,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(22,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(23,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(24,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(25,:) = (/ t%tev%XS_tthj_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%tev%XS_ttH_SM(j) , t%BR_HWW_SM(j) /) channel_SM(6,:) = (/ t%tev%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(7,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(8,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(9,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(10,:) = (/ t%tev%XS_ttH_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(11,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(12,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(13,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(14,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(15,:) = (/ t%tev%XS_ttH_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(16,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(17,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(18,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(19,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(20,:) = (/ t%tev%XS_ttH_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(21,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(22,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(23,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(24,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(25,:) = (/ t%tev%XS_ttH_SM(j) , t%BR_Hbb_SM(j) /) case(6183,3233) ! ns = 4; nb = 4; call initialise_XS_rat_BR_rat nc = 16; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hj_ratio(j) ! XS_rat(3) = t%tev%XS_hjZ_ratio(j) ! XS_rat(4) = t%tev%XS_vbf_ratio(j) ! BR_rat(1) = div(t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div( t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) ! BR_rat(3) = div(t%BR_hjtautau(j) , t%BR_Htautau_SM(j) ,0.0D0,1.0D0) ! BR_rat(4) = div(t%BR_hjgaga(j) , t%BR_Hgaga_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(11,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(12,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(13,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(14,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(15,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(16,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%tev%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(6,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(7,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(8,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(9,:) = (/ t%tev%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(10,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(11,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(12,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(13,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(14,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(15,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(16,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hgaga_SM(j) /) case(6286) ! ns = 4; nb = 4; call initialise_XS_rat_BR_rat nc = 9; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjmumu(j),t%BR_Hmumu_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j), t%BR_HZZ_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(6,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(7,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HWW_SM(j) /) channel_SM(8,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(9,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hmumu_SM(j) /) case(6305) ! ns = 4; nb = 3; call initialise_XS_rat_BR_rat nc = 12; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hj_ratio(j) ! XS_rat(3) = t%tev%XS_hjZ_ratio(j) ! XS_rat(4) = t%tev%XS_vbf_ratio(j) ! BR_rat(1) = div(t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div( t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) ! BR_rat(3) = div(t%BR_hjtautau(j) , t%BR_Htautau_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(11,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(12,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%tev%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(6,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(7,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(8,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(9,:) = (/ t%tev%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(10,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(11,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(12,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HZZ_SM(j) /) case(6096,10606,10806,10884) nc = 30; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%tev%XS_tthj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%tev%XS_tthj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(11,:) = (/ t%tev%XS_hj_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(12,:) = (/ t%tev%XS_vbf_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(13,:) = (/ t%tev%XS_hjW_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(14,:) = (/ t%tev%XS_hjZ_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(15,:) = (/ t%tev%XS_tthj_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(16,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(17,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(18,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(19,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(20,:) = (/ t%tev%XS_tthj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(21,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(22,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(23,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(24,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(25,:) = (/ t%tev%XS_tthj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(26,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(27,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(28,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(29,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(30,:) = (/ t%tev%XS_tthj_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%tev%XS_ttH_SM(j) , t%BR_HWW_SM(j) /) channel_SM(6,:) = (/ t%tev%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(7,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(8,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(9,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(10,:) = (/ t%tev%XS_ttH_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(11,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(12,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(13,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(14,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(15,:) = (/ t%tev%XS_ttH_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(16,:) = (/ t%tev%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(17,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(18,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(19,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(20,:) = (/ t%tev%XS_ttH_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(21,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(22,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(23,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(24,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(25,:) = (/ t%tev%XS_ttH_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(26,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(27,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(28,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(29,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(30,:) = (/ t%tev%XS_ttH_SM(j) , t%BR_Hbb_SM(j) /) case(6229) ! ns = 4; nb = 6; call initialise_XS_rat_BR_rat nc = 24; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hj_ratio(j) ! XS_rat(3) = t%tev%XS_hjZ_ratio(j) ! XS_rat(4) = t%tev%XS_vbf_ratio(j) ! BR_rat(1) = div( t%BR_hjbb(j) , t%BR_Hbb_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(3) = div(t%BR_hjtautau(j) , t%BR_Htautau_SM(j) ,0.0D0,1.0D0) ! BR_rat(4) = div( t%BR_hjgaga(j) , t%BR_Hgaga_SM(j) ,0.0D0,1.0D0) ! BR_rat(5) = div(( t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j) ) & ! & , t%BR_Hjets_SM(j) ,0.0D0,1.0D0) ! BR_rat(6) = div( t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%tev%XS_hj_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%tev%XS_vbf_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(11,:) = (/ t%tev%XS_hjW_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(12,:) = (/ t%tev%XS_hjZ_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(13,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(14,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(15,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(16,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(17,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(18,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(19,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(20,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(21,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(22,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(23,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(24,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%tev%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(6,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(7,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(8,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(9,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(10,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(11,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(12,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(13,:) = (/ t%tev%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(14,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(15,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(16,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(17,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(18,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(19,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(20,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(21,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(22,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(23,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(24,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hbb_SM(j) /) case(6304) ! ns = 4; nb = 5; call initialise_XS_rat_BR_rat nc = 20; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(11,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(12,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(13,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(14,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(15,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(16,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(17,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(18,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(19,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(20,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%tev%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(6,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(7,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(8,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(9,:) = (/ t%tev%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(10,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(11,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(12,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(13,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(14,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(15,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(16,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(17,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(18,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(19,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(20,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hbb_SM(j) /) case(6171) ! ns = 4; nb = 3; call initialise_XS_rat_BR_rat nc = 12; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hj_ratio(j) ! XS_rat(3) = t%tev%XS_hjZ_ratio(j) ! XS_rat(4) = t%tev%XS_vbf_ratio(j) ! BR_rat(1) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div(t%BR_hjtautau(j) , t%BR_Htautau_SM(j),0.0D0,1.0D0) ! BR_rat(3) = div(( t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j) ) & ! & , t%BR_Hjets_SM(j),0.0D0,1.0D0) channel_rat(1,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%tev%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%tev%XS_vbf_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%tev%XS_hjW_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%tev%XS_hjZ_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%tev%XS_hj_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%tev%XS_vbf_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(11,:) = (/ t%tev%XS_hjW_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_rat(12,:) = (/ t%tev%XS_hjZ_ratio(j) , & & div((t%BR_hjss(j)+t%BR_hjcc(j)+t%BR_hjbb(j)+t%BR_hjgg(j)),t%BR_Hjets_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%tev%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%tev%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%tev%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(6,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(7,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(8,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(9,:) = (/ t%tev%XS_H_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(10,:) = (/ t%tev%XS_vbf_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(11,:) = (/ t%tev%XS_HW_SM(j) , t%BR_Hjets_SM(j) /) channel_SM(12,:) = (/ t%tev%XS_HZ_SM(j) , t%BR_Hjets_SM(j) /) !---------------------- LHC 7/8 TeV searches -------------------- case(5757,2011005,3615,2012018) ! ns = 2; nb = 1; call initialise_XS_rat_BR_rat nc = 2; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hj_ratio(j) ! XS_rat(2) = t%tev%XS_vbf_ratio(j) ! BR_rat(1) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HWW_SM(j) /) case(12046) nc = 2; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_HWW_SM(j) /) case(2011048,11004,11015,11013,11028,11006,11017,110271,110272,14161,14162,5064,2012017,2011150,2011131) ! ns = 2; nb = 1; call initialise_XS_rat_BR_rat nc = 2; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hj_ratio(j) ! XS_rat(2) = t%lhc7%XS_vbf_ratio(j) ! BR_rat(1) = div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j) , t%BR_HZZ_SM(j) /) case(11034,12039,13009,12006,2012078) ! ns = 1; nb = 2; call initialise_XS_rat_BR_rat nc = 2; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc7%XS_hjW_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_hjW_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_HW_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_HW_SM(j) , t%BR_Htautau_SM(j) /) case(12051) nc = 2; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc7%XS_hjW_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_hjZ_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_HW_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_HZ_SM(j) , t%BR_Htautau_SM(j) /) case(2012015) ! ns = 2; nb = 1; call initialise_XS_rat_BR_rat nc = 2; call initialise_channel_rat_SM ! XS_rat(1) = t%tev%XS_hjW_ratio(j) ! XS_rat(2) = t%tev%XS_hjZ_ratio(j) ! BR_rat(1) = div(t%BR_hjbb(j) , t%BR_Hbb_SM(j),0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hjW_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_hjZ_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_HW_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_HZ_SM(j) , t%BR_Hbb_SM(j) /) case(2011162,1415) ! ns = 4; nb = 1; call initialise_XS_rat_BR_rat nc = 4; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hj_ratio(j) ! XS_rat(2) = t%lhc7%XS_vbf_ratio(j) ! XS_rat(3) = t%lhc7%XS_hjZ_ratio(j) ! XS_rat(4) = t%lhc7%XS_hjW_ratio(j) ! BR_rat(1) = div(t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HZZ_SM(j) /) channel_SM(3,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_HZZ_SM(j) /) channel_SM(4,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_HZZ_SM(j) /) case(2012092,20130131) nc = 4; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(2,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_HZZ_SM(j) /) channel_SM(3,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_HZZ_SM(j) /) channel_SM(4,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_HZZ_SM(j) /) case(11025,1997) ! ns = 5; nb = 1; call initialise_XS_rat_BR_rat nc = 5; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hj_ratio(j) ! XS_rat(2) = t%lhc7%XS_vbf_ratio(j) ! XS_rat(3) = t%lhc7%XS_hjZ_ratio(j) ! XS_rat(4) = t%lhc7%XS_hjW_ratio(j) ! XS_rat(5) = t%lhc7%XS_tthj_ratio(j) ! BR_rat(1) = div(t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HZZ_SM(j) /) channel_SM(3,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_HZZ_SM(j) /) channel_SM(4,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_HZZ_SM(j) /) channel_SM(5,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_HZZ_SM(j) /) case(12041,130021,130022) nc = 5; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%lhc8%XS_tthj_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(2,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_HZZ_SM(j) /) channel_SM(3,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_HZZ_SM(j) /) channel_SM(4,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_HZZ_SM(j) /) channel_SM(5,:) = (/ t%lhc8%XS_ttH_SM(j), t%BR_HZZ_SM(j) /) case(2011026,11005,11016,11026,3478,3357,2011148,2012016) ! ns = 2; nb = 2; call initialise_XS_rat_BR_rat nc = 4; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hj_ratio(j) ! XS_rat(2) = t%lhc7%XS_vbf_ratio(j) ! BR_rat(1) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div(t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(4,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HZZ_SM(j) /) case(11003,11014,2577,11024,1489) ! ns = 5; nb = 2; call initialise_XS_rat_BR_rat nc = 10; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hj_ratio(j) ! XS_rat(2) = t%lhc7%XS_vbf_ratio(j) ! XS_rat(3) = t%lhc7%XS_hjZ_ratio(j) ! XS_rat(4) = t%lhc7%XS_hjW_ratio(j) ! XS_rat(5) = t%lhc7%XS_tthj_ratio(j) ! BR_rat(1) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div( t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_HWW_SM(j) /) channel_SM(6,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(7,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HZZ_SM(j) /) channel_SM(8,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_HZZ_SM(j) /) channel_SM(9,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_HZZ_SM(j) /) channel_SM(10,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_HZZ_SM(j) /) case(12042,13003,13027) nc = 4; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hj_ratio(j) ! XS_rat(2) = t%lhc7%XS_vbf_ratio(j) ! XS_rat(3) = t%lhc7%XS_hjZ_ratio(j) ! XS_rat(4) = t%lhc7%XS_hjW_ratio(j) ! XS_rat(5) = t%lhc7%XS_tthj_ratio(j) ! BR_rat(1) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div( t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_HWW_SM(j) /) case(2012014) ! ns = 5; nb = 1; call initialise_XS_rat_BR_rat nc = 5; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hj_ratio(j) ! XS_rat(2) = t%lhc7%XS_vbf_ratio(j) ! XS_rat(3) = t%lhc7%XS_hjZ_ratio(j) ! XS_rat(4) = t%lhc7%XS_hjW_ratio(j) ! XS_rat(5) = t%lhc7%XS_tthj_ratio(j) ! BR_rat(1) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div( t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Htautau_SM(j) /) channel_SM(3,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_Htautau_SM(j) /) channel_SM(4,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_Htautau_SM(j) /) channel_SM(5,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_Htautau_SM(j) /) case(2012160) ! ns = 5; nb = 1; call initialise_XS_rat_BR_rat nc = 4; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hj_ratio(j) ! XS_rat(2) = t%lhc7%XS_vbf_ratio(j) ! XS_rat(3) = t%lhc7%XS_hjZ_ratio(j) ! XS_rat(4) = t%lhc7%XS_hjW_ratio(j) ! XS_rat(5) = t%lhc7%XS_tthj_ratio(j) ! BR_rat(1) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div( t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Htautau_SM(j) /) channel_SM(3,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_Htautau_SM(j) /) channel_SM(4,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_Htautau_SM(j) /) case(11009,11020,2011133) ! ns = 2; nb = 1; call initialise_XS_rat_BR_rat nc = 2; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hj_ratio(j) ! XS_rat(2) = t%lhc7%XS_vbf_ratio(j) ! BR_rat(1) = div( t%BR_hjtautau(j) , t%BR_Htautau_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Htautau_SM(j) /) case(110291) ! ns = 5; nb = 1; call initialise_XS_rat_BR_rat nc = 5; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hj_ratio(j) ! XS_rat(2) = t%lhc7%XS_vbf_ratio(j) ! XS_rat(3) = t%lhc7%XS_hjZ_ratio(j) ! XS_rat(4) = t%lhc7%XS_hjW_ratio(j) ! XS_rat(5) = t%lhc7%XS_tthj_ratio(j) ! BR_rat(1) = div( t%BR_hjtautau(j) , t%BR_Htautau_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Htautau_SM(j) /) channel_SM(3,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_Htautau_SM(j) /) channel_SM(4,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_Htautau_SM(j) /) channel_SM(5,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_Htautau_SM(j) /) case(12043) nc = 4; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(2,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_Htautau_SM(j) /) channel_SM(3,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_Htautau_SM(j) /) channel_SM(4,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_Htautau_SM(j) /) case(2013010,7663) nc = 4; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjmumu(j),t%BR_Hmumu_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjmumu(j),t%BR_Hmumu_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjmumu(j),t%BR_Hmumu_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjmumu(j),t%BR_Hmumu_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_Hmumu_SM(j) /) channel_SM(2,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_Hmumu_SM(j) /) channel_SM(3,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_Hmumu_SM(j) /) channel_SM(4,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_Hmumu_SM(j) /) case(11031,2011103,11012) nc = 2; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_Hbb_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_Hbb_SM(j) /) case(12044,13012) nc = 2; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_Hbb_SM(j) /) channel_SM(2,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_Hbb_SM(j) /) case(13011) nc = 2; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(2,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_Hbb_SM(j) /) case(2012161) nc = 2; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_Hbb_SM(j) /) channel_SM(2,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_Hbb_SM(j) /) case(11021) ! ns = 2; nb = 1; call initialise_XS_rat_BR_rat nc = 2; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hj_ratio(j) ! XS_rat(2) = t%lhc7%XS_vbf_ratio(j) ! BR_rat(1) = div( t%BR_hjgaga(j) , t%BR_Hgaga_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Hgaga_SM(j) /) case(110212) ! ns = 3; nb = 1; call initialise_XS_rat_BR_rat nc = 3; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_vbf_ratio(j) ! XS_rat(2) = t%lhc7%XS_hjZ_ratio(j) ! XS_rat(3) = t%lhc7%XS_hjW_ratio(j) ! BR_rat(1) = div( t%BR_hjgaga(j) , t%BR_Hgaga_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(3,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_Hgaga_SM(j) /) case(2011025,2011085,2011161,5895,1414,1487,12001,11010,11030) ! ns = 5; nb = 1; call initialise_XS_rat_BR_rat nc = 5; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hj_ratio(j) ! XS_rat(2) = t%lhc7%XS_vbf_ratio(j) ! XS_rat(3) = t%lhc7%XS_hjZ_ratio(j) ! XS_rat(4) = t%lhc7%XS_hjW_ratio(j) ! XS_rat(5) = t%lhc7%XS_tthj_ratio(j) ! BR_rat(1) = div( t%BR_hjgaga(j) , t%BR_Hgaga_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(3,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(4,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(5,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_Hgaga_SM(j) /) + case(17013) + nc = 5; call initialise_channel_rat_SM + + channel_rat(1,:) = (/ t%lhc13%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) + channel_rat(2,:) = (/ t%lhc13%XS_vbf_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) + channel_rat(3,:) = (/ t%lhc13%XS_hjZ_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) + channel_rat(4,:) = (/ t%lhc13%XS_hjW_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) + channel_rat(5,:) = (/ t%lhc13%XS_tthj_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) + + channel_SM(1,:) = (/ t%lhc13%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) + channel_SM(2,:) = (/ t%lhc13%XS_vbf_SM(j), t%BR_Hgaga_SM(j) /) + channel_SM(3,:) = (/ t%lhc13%XS_HZ_SM(j), t%BR_Hgaga_SM(j) /) + channel_SM(4,:) = (/ t%lhc13%XS_HW_SM(j), t%BR_Hgaga_SM(j) /) + channel_SM(5,:) = (/ t%lhc13%XS_ttH_SM(j), t%BR_Hgaga_SM(j) /) + + case(2012091,2012168) ! ns = 5; nb = 1; call initialise_XS_rat_BR_rat nc = 5; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%lhc8%XS_tthj_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(2,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(3,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(4,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(5,:) = (/ t%lhc8%XS_ttH_SM(j), t%BR_Hgaga_SM(j) /) case(12015,13001) nc = 5; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%lhc8%XS_tthj_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(2,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(3,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(4,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(5,:) = (/ t%lhc8%XS_ttH_SM(j), t%BR_Hgaga_SM(j) /) case(13006,13075515,2013009,3051) nc = 5; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hj_ratio(j) ! XS_rat(2) = t%lhc7%XS_vbf_ratio(j) ! XS_rat(3) = t%lhc7%XS_hjZ_ratio(j) ! XS_rat(4) = t%lhc7%XS_hjW_ratio(j) ! XS_rat(5) = t%lhc7%XS_tthj_ratio(j) ! BR_rat(1) = div( t%BR_hjgaga(j) , t%BR_Hgaga_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjZga(j),t%BR_HZga_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjZga(j),t%BR_HZga_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjZga(j),t%BR_HZga_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjZga(j),t%BR_HZga_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%lhc8%XS_tthj_ratio(j), div(t%BR_hjZga(j),t%BR_HZga_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_HZga_SM(j) /) channel_SM(2,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_HZga_SM(j) /) channel_SM(3,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_HZga_SM(j) /) channel_SM(4,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_HZga_SM(j) /) channel_SM(5,:) = (/ t%lhc8%XS_ttH_SM(j), t%BR_HZga_SM(j) /) case(2748, 1408) ! ns = 5; nb = 3; call initialise_XS_rat_BR_rat nc = 15; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hjW_ratio(j) ! XS_rat(2) = t%lhc7%XS_hj_ratio(j) ! XS_rat(3) = t%lhc7%XS_hjZ_ratio(j) ! XS_rat(4) = t%lhc7%XS_vbf_ratio(j) ! XS_rat(5) = t%lhc7%XS_tthj_ratio(j) ! BR_rat(1) = div( t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(3) = div( t%BR_hjgaga(j) , t%BR_Hgaga_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(11,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(12,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(13,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(14,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(15,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_HWW_SM(j) /) channel_SM(6,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(7,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HZZ_SM(j) /) channel_SM(8,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_HZZ_SM(j) /) channel_SM(9,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_HZZ_SM(j) /) channel_SM(10,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_HZZ_SM(j) /) channel_SM(11,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(12,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(13,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(14,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(15,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_Hgaga_SM(j) /) case(11011,2011163) ! ns = 5; nb = 4; call initialise_XS_rat_BR_rat nc = 20; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hjW_ratio(j) ! XS_rat(2) = t%lhc7%XS_hj_ratio(j) ! XS_rat(3) = t%lhc7%XS_hjZ_ratio(j) ! XS_rat(4) = t%lhc7%XS_vbf_ratio(j) ! XS_rat(5) = t%lhc7%XS_tthj_ratio(j) ! BR_rat(1) = div( t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(3) = div( t%BR_hjgaga(j) , t%BR_Hgaga_SM(j) ,0.0D0,1.0D0) ! BR_rat(4) = div(t%BR_hjtautau(j) , t%BR_Htautau_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(11,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(12,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(13,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(14,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(15,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(16,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(17,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(18,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(19,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(20,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_HWW_SM(j) /) channel_SM(6,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(7,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HZZ_SM(j) /) channel_SM(8,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_HZZ_SM(j) /) channel_SM(9,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_HZZ_SM(j) /) channel_SM(10,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_HZZ_SM(j) /) channel_SM(11,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(12,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(13,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(14,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(15,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(16,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(17,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Htautau_SM(j) /) channel_SM(18,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_Htautau_SM(j) /) channel_SM(19,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_Htautau_SM(j) /) channel_SM(20,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_Htautau_SM(j) /) case(2012012) ! ns = 2; nb = 1; call initialise_XS_rat_BR_rat nc = 2; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HWW_SM(j) /) case(2012158,2013030) ! ns = 2; nb = 1; call initialise_XS_rat_BR_rat nc = 4; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_HWW_SM(j) /) case(2012135,12025) nc = 1; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_Hbb_SM(j) /) case(2011112) ! ns = 5; nb = 4; call initialise_XS_rat_BR_rat nc = 20; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hjW_ratio(j) ! XS_rat(2) = t%lhc7%XS_hj_ratio(j) ! XS_rat(3) = t%lhc7%XS_hjZ_ratio(j) ! XS_rat(4) = t%lhc7%XS_vbf_ratio(j) ! XS_rat(5) = t%lhc7%XS_tthj_ratio(j) ! BR_rat(1) = div( t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(3) = div( t%BR_hjgaga(j) , t%BR_Hgaga_SM(j) ,0.0D0,1.0D0) ! BR_rat(4) = div( t%BR_hjbb(j) , t%BR_Hbb_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(11,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(12,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(13,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(14,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(15,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(16,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(17,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(18,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(19,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(20,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_HWW_SM(j) /) channel_SM(6,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(7,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HZZ_SM(j) /) channel_SM(8,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_HZZ_SM(j) /) channel_SM(9,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_HZZ_SM(j) /) channel_SM(10,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_HZZ_SM(j) /) channel_SM(11,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(12,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(13,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(14,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(15,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(16,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(17,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Hbb_SM(j) /) channel_SM(18,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_Hbb_SM(j) /) channel_SM(19,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_Hbb_SM(j) /) channel_SM(20,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_Hbb_SM(j) /) case(11022,11032,1488,12008,2011157,2012019,2011135) ! ns = 5; nb = 5; call initialise_XS_rat_BR_rat nc = 25; call initialise_channel_rat_SM ! XS_rat(1) = t%lhc7%XS_hj_ratio(j) ! XS_rat(2) = t%lhc7%XS_vbf_ratio(j) ! XS_rat(1) = t%lhc7%XS_hjW_ratio(j) ! XS_rat(3) = t%lhc7%XS_hjZ_ratio(j) ! XS_rat(5) = t%lhc7%XS_tthj_ratio(j) ! BR_rat(1) = div( t%BR_hjZZ(j) , t%BR_HZZ_SM(j) ,0.0D0,1.0D0) ! BR_rat(2) = div( t%BR_hjWW(j) , t%BR_HWW_SM(j) ,0.0D0,1.0D0) ! BR_rat(3) = div( t%BR_hjgaga(j) , t%BR_Hgaga_SM(j) ,0.0D0,1.0D0) ! BR_rat(4) = div(t%BR_hjtautau(j) , t%BR_Htautau_SM(j) ,0.0D0,1.0D0) ! BR_rat(5) = div( t%BR_hjbb(j) , t%BR_Hbb_SM(j) ,0.0D0,1.0D0) channel_rat(1,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(11,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(12,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(13,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(14,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(15,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(16,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(17,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(18,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(19,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(20,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(21,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(22,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(23,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(24,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(25,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_HWW_SM(j) /) channel_SM(6,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(7,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_HZZ_SM(j) /) channel_SM(8,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_HZZ_SM(j) /) channel_SM(9,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_HZZ_SM(j) /) channel_SM(10,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_HZZ_SM(j) /) channel_SM(11,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(12,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(13,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(14,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(15,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(16,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(17,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Htautau_SM(j) /) channel_SM(18,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_Htautau_SM(j) /) channel_SM(19,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_Htautau_SM(j) /) channel_SM(20,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_Htautau_SM(j) /) channel_SM(21,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(22,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Hbb_SM(j) /) channel_SM(23,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_Hbb_SM(j) /) channel_SM(24,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_Hbb_SM(j) /) channel_SM(25,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_Hbb_SM(j) /) case(12045) nc = 25; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%lhc8%XS_tthj_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%lhc8%XS_tthj_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(11,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(12,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(13,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(14,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(15,:) = (/ t%lhc8%XS_tthj_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(16,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(17,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(18,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(19,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(20,:) = (/ t%lhc8%XS_tthj_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(21,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(22,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(23,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(24,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(25,:) = (/ t%lhc8%XS_tthj_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%lhc8%XS_ttH_SM(j), t%BR_HWW_SM(j) /) channel_SM(6,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(7,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_HZZ_SM(j) /) channel_SM(8,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_HZZ_SM(j) /) channel_SM(9,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_HZZ_SM(j) /) channel_SM(10,:) = (/ t%lhc8%XS_ttH_SM(j), t%BR_HZZ_SM(j) /) channel_SM(11,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(12,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(13,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(14,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(15,:) = (/ t%lhc8%XS_ttH_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(16,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(17,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_Htautau_SM(j) /) channel_SM(18,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_Htautau_SM(j) /) channel_SM(19,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_Htautau_SM(j) /) channel_SM(20,:) = (/ t%lhc8%XS_ttH_SM(j), t%BR_Htautau_SM(j) /) channel_SM(21,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(22,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_Hbb_SM(j) /) channel_SM(23,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_Hbb_SM(j) /) channel_SM(24,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_Hbb_SM(j) /) channel_SM(25,:) = (/ t%lhc8%XS_ttH_SM(j), t%BR_Hbb_SM(j) /) case(009361) nc = 10; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%lhc8%XS_tthj_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%lhc8%XS_tthj_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%lhc8%XS_ttH_SM(j), t%BR_HWW_SM(j) /) channel_SM(6,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(7,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_HZZ_SM(j) /) channel_SM(8,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_HZZ_SM(j) /) channel_SM(9,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_HZZ_SM(j) /) channel_SM(10,:) = (/ t%lhc8%XS_ttH_SM(j), t%BR_HZZ_SM(j) /) case(17020321,17020322,17020323) ! This only checks the relative proportions of the four main production modes nc = 4; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc8%XS_hj_ratio(j) , 1.0D0 /) channel_rat(2,:) = (/ t%lhc8%XS_vbf_ratio(j), 1.0D0 /) channel_rat(3,:) = (/ t%lhc8%XS_hjZ_ratio(j), 1.0D0 /) channel_rat(4,:) = (/ t%lhc8%XS_hjW_ratio(j), 1.0D0 /) channel_SM(1,:) = (/ t%lhc8%XS_H_SM(j) , 1.0D0 /) channel_SM(2,:) = (/ t%lhc8%XS_vbf_SM(j), 1.0D0 /) channel_SM(3,:) = (/ t%lhc8%XS_HZ_SM(j), 1.0D0 /) channel_SM(4,:) = (/ t%lhc8%XS_HW_SM(j), 1.0D0 /) + + case(539) +! This only checks the relative proportions of the four main production modes + nc = 4; call initialise_channel_rat_SM + channel_rat(1,:) = (/ t%lhc13%XS_hj_ratio(j) , 1.0D0 /) + channel_rat(2,:) = (/ t%lhc13%XS_vbf_ratio(j), 1.0D0 /) + channel_rat(3,:) = (/ t%lhc13%XS_hjZ_ratio(j), 1.0D0 /) + channel_rat(4,:) = (/ t%lhc13%XS_hjW_ratio(j), 1.0D0 /) + + channel_SM(1,:) = (/ t%lhc13%XS_H_SM(j) , 1.0D0 /) + channel_SM(2,:) = (/ t%lhc13%XS_vbf_SM(j), 1.0D0 /) + channel_SM(3,:) = (/ t%lhc13%XS_HZ_SM(j), 1.0D0 /) + channel_SM(4,:) = (/ t%lhc13%XS_HW_SM(j), 1.0D0 /) case(7214) nc = 25; call initialise_channel_rat_SM channel_rat(1,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(2,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(3,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(4,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(5,:) = (/ t%lhc8%XS_tthj_ratio(j), div(t%BR_hjWW(j),t%BR_HWW_SM(j),0.0D0,1.0D0) /) channel_rat(6,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(7,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(8,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(9,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(10,:) = (/ t%lhc8%XS_tthj_ratio(j), div(t%BR_hjZZ(j),t%BR_HZZ_SM(j),0.0D0,1.0D0) /) channel_rat(11,:) = (/ t%lhc8%XS_hj_ratio(j) , div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(12,:) = (/ t%lhc8%XS_vbf_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(13,:) = (/ t%lhc8%XS_hjZ_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(14,:) = (/ t%lhc8%XS_hjW_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(15,:) = (/ t%lhc8%XS_tthj_ratio(j), div(t%BR_hjgaga(j),t%BR_Hgaga_SM(j),0.0D0,1.0D0) /) channel_rat(16,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(17,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(18,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(19,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(20,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjtautau(j),t%BR_Htautau_SM(j),0.0D0,1.0D0) /) channel_rat(21,:) = (/ t%lhc7%XS_hj_ratio(j) , div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(22,:) = (/ t%lhc7%XS_vbf_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(23,:) = (/ t%lhc7%XS_hjZ_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(24,:) = (/ t%lhc7%XS_hjW_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_rat(25,:) = (/ t%lhc7%XS_tthj_ratio(j), div(t%BR_hjbb(j),t%BR_Hbb_SM(j),0.0D0,1.0D0) /) channel_SM(1,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_HWW_SM(j) /) channel_SM(2,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_HWW_SM(j) /) channel_SM(3,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_HWW_SM(j) /) channel_SM(4,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_HWW_SM(j) /) channel_SM(5,:) = (/ t%lhc8%XS_ttH_SM(j), t%BR_HWW_SM(j) /) channel_SM(6,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_HZZ_SM(j) /) channel_SM(7,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_HZZ_SM(j) /) channel_SM(8,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_HZZ_SM(j) /) channel_SM(9,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_HZZ_SM(j) /) channel_SM(10,:) = (/ t%lhc8%XS_ttH_SM(j), t%BR_HZZ_SM(j) /) channel_SM(11,:) = (/ t%lhc8%XS_H_SM(j) , t%BR_Hgaga_SM(j) /) channel_SM(12,:) = (/ t%lhc8%XS_vbf_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(13,:) = (/ t%lhc8%XS_HZ_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(14,:) = (/ t%lhc8%XS_HW_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(15,:) = (/ t%lhc8%XS_ttH_SM(j), t%BR_Hgaga_SM(j) /) channel_SM(16,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_Htautau_SM(j) /) channel_SM(17,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Htautau_SM(j) /) channel_SM(18,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_Htautau_SM(j) /) channel_SM(19,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_Htautau_SM(j) /) channel_SM(20,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_Htautau_SM(j) /) channel_SM(21,:) = (/ t%lhc7%XS_H_SM(j) , t%BR_Hbb_SM(j) /) channel_SM(22,:) = (/ t%lhc7%XS_vbf_SM(j), t%BR_Hbb_SM(j) /) channel_SM(23,:) = (/ t%lhc7%XS_HZ_SM(j), t%BR_Hbb_SM(j) /) channel_SM(24,:) = (/ t%lhc7%XS_HW_SM(j), t%BR_Hbb_SM(j) /) channel_SM(25,:) = (/ t%lhc7%XS_ttH_SM(j), t%BR_Hbb_SM(j) /) case(5739,10574) ns = 1; nb = 1; call initialise_XS_rat_BR_rat XS_rat(1) = t%tev%XS_tthj_ratio(j) BR_rat(1) = div(t%BR_hjbb(j) , t%BR_Hbb_SM(j) ,0.0D0,1.0D0) if(t%CP_value(j).eq.1)then ! analysis only applies if higgs is CP even else correct_properties=.False. endif case(711) ns = 1; nb = 1; call initialise_XS_rat_BR_rat XS_rat(1) = t%lep%XS_bbhj_ratio(j) BR_rat(1) = t%BR_hjbb(j) !note *not* normalised to SM if(t%CP_value(j).eq.1)then ! analysis only applies if higgs is CP even else correct_properties=.False. endif case(713) ns = 1; nb = 1; call initialise_XS_rat_BR_rat XS_rat(1) = t%lep%XS_bbhj_ratio(j) BR_rat(1) = t%BR_hjbb(j)!note *not* normalised to SM if(t%CP_value(j).eq.-1)then ! analysis only applies if higgs is CP odd else correct_properties=.False. endif case(721) ns = 1; nb = 1; call initialise_XS_rat_BR_rat XS_rat(1) = t%lep%XS_bbhj_ratio(j) BR_rat(1) = t%BR_hjtautau(j)!note *not* normalised to SM if(t%CP_value(j).eq.1)then ! analysis only applies if higgs is CP even else correct_properties=.False. endif case(723) ns = 1; nb = 1; call initialise_XS_rat_BR_rat XS_rat(1) = t%lep%XS_bbhj_ratio(j) BR_rat(1) = t%BR_hjtautau(j)!note *not* normalised to SM if(t%CP_value(j).eq.-1)then ! analysis only applies if higgs is CP odd else correct_properties=.False. endif case(731) ns = 1; nb = 1; call initialise_XS_rat_BR_rat XS_rat(1) = t%lep%XS_tautauhj_ratio(j) BR_rat(1) = t%BR_hjtautau(j)!note *not* normalised to SM if(t%CP_value(j).eq.1)then ! analysis only applies if higgs is CP even else correct_properties=.False. endif case(733) ns = 1; nb = 1; call initialise_XS_rat_BR_rat XS_rat(1) = t%lep%XS_tautauhj_ratio(j) BR_rat(1) = t%BR_hjtautau(j)!note *not* normalised to SM if(t%CP_value(j).eq.-1)then ! analysis only applies if higgs is CP odd else correct_properties=.False. endif case(741) ns = 1; nb = 1; call initialise_XS_rat_BR_rat XS_rat(1) = t%lep%XS_bbhj_ratio(j) BR_rat(1) = t%BR_hjtautau(j)!note *not* normalised to SM if(t%CP_value(j).eq.1)then ! analysis only applies if higgs is CP even else correct_properties=.False. endif case(743) ns = 1; nb = 1; call initialise_XS_rat_BR_rat XS_rat(1) = t%lep%XS_bbhj_ratio(j) BR_rat(1) = t%BR_hjtautau(j)!note *not* normalised to SM if(t%CP_value(j).eq.-1)then ! analysis only applies if higgs is CP odd else correct_properties=.False. endif case(1811,2011094,13035) ns = 1; nb = 1; call initialise_XS_rat_BR_rat XS_rat(1) = t%BR_tHpjb(j) BR_rat(1) = t%BR_Hpjcs(j) if( (t%BR_tHpjb(j)+t%BR_tWpb ).le.0.98D0)then correct_properties=.False. elseif((t%BR_Hpjcs(j)+t%BR_Hpjtaunu(j)).le.0.98D0)then correct_properties=.False. endif case(1812,7712,8353,11002,11008,160311) ns = 1; nb = 1; call initialise_XS_rat_BR_rat XS_rat(1) = t%BR_tHpjb(j) BR_rat(1) = t%BR_Hpjtaunu(j) if( (t%BR_tHpjb(j)+t%BR_tWpb).le.0.98D0)then correct_properties=.False. elseif((t%BR_Hpjcs(j)+t%BR_Hpjtaunu(j)).le.0.98D0)then correct_properties=.False. endif case(2011138,2011151,2760,2013090,2014050,14020,79152) ns = 1; nb = 1; call initialise_XS_rat_BR_rat XS_rat(1) = t%BR_tHpjb(j) BR_rat(1) = t%BR_Hpjtaunu(j) if( (t%BR_tHpjb(j)+t%BR_tWpb).le.0.98D0)then correct_properties=.False. endif case(1269,1270) ns = 1; nb = 1; call initialise_XS_rat_BR_rat XS_rat(1) = t%BR_tHpjb(j) BR_rat(1) = t%BR_Hpjcs(j) if( (t%BR_tHpjb(j)+t%BR_tWpb ).le.0.98D0)then correct_properties=.False. elseif( t%BR_Hpjcs(j) .le.0.98D0)then correct_properties=.False. endif case(6224) ns = 1; nb = 1; call initialise_XS_rat_BR_rat XS_rat(1) = t%tev%XS_hjb_ratio(j)*t%tev%XS_Hb_c4_SM(j) BR_rat(1) = 1.0D0 if( ( t%BR_hjtautau(j)+t%BR_hjbb(j) ).le.0.98D0)then correct_properties=.False. elseif( t%BR_hjtautau(j) .le.0.06D0)then correct_properties=.False. endif case(6225) ns = 1; nb = 1; call initialise_XS_rat_BR_rat XS_rat(1) = t%tev%XS_hjb_ratio(j)*t%tev%XS_Hb_c4_SM(j) BR_rat(1) = 1.0D0 if( ( t%BR_hjtautau(j)+t%BR_hjbb(j) ).le.0.98D0)then correct_properties=.False. elseif( t%BR_hjtautau(j) .le.0.1D0)then correct_properties=.False. endif case(6226) ns = 1; nb = 1; call initialise_XS_rat_BR_rat XS_rat(1) = t%tev%XS_hjb_ratio(j)*t%tev%XS_Hb_c4_SM(j) BR_rat(1) = 1.0D0 if( ( t%BR_hjtautau(j)+t%BR_hjbb(j) ).le.0.98D0)then correct_properties=.False. elseif( t%BR_hjtautau(j) .le.0.14D0)then correct_properties=.False. endif case(04670) ! This is a H->h(SM)h(SM) search! ns = 1; nb =1; call initialise_XS_rat_BR_rat XS_rat(1) = t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j) BR_rat(1) = 0.0D0 correct_properties=.False. do jj=1,np(Hneut) if(abs(t%particle(Hneut)%M(jj)-125.4).lt.(5.0D0+t%particle(Hneut)%dMh(jj))) then dcbyc_dble=maxval((/ div(abs(t%BR_hjgaga(jj)-t%BR_Hgaga_SM(jj)),t%BR_Hgaga_SM(jj),0.0D0,1.0D0),& & div(abs(t%BR_hjWW(jj)-t%BR_HWW_SM(jj)),t%BR_HWW_SM(jj),0.0D0,1.0D0), & & div(abs(t%BR_hjbb(jj)-t%BR_Hbb_SM(jj)),t%BR_Hbb_SM(jj),0.0D0,1.0D0), & & div(abs(t%BR_hjtautau(jj)-t%BR_Htautau_SM(jj)),t%BR_Htautau_SM(jj),0.0D0,1.0D0) /)) if(dcbyc_dble.lt.0.1D0) then correct_properties=.True. BR_rat(1) = BR_rat(1)+t%BR_hjhihi(j,jj) endif endif enddo case(17030) ! This is a H->h(SM)h(SM) search! ! n.b.: In principle, should also check for SM strength of h production modes, as this ! is part of the assumed background! ns = 1; nb =1; call initialise_XS_rat_BR_rat XS_rat(1) = 1000.0D0 * t%lhc13%XS_hj_ratio(j)*t%lhc13%XS_H_SM(j) ! convert to fb BR_rat(1) = 0.0D0 correct_properties=.False. do jj=1,np(Hneut) if(abs(t%particle(Hneut)%M(jj)-125.0D0).lt.(5.0D0+t%particle(Hneut)%dMh(jj))) then dcbyc_dble=maxval((/ div(abs(t%BR_hjgaga(jj)-t%BR_Hgaga_SM(jj)),t%BR_Hgaga_SM(jj),0.0D0,1.0D0),& & div(abs(t%BR_hjWW(jj)-t%BR_HWW_SM(jj)),t%BR_HWW_SM(jj),0.0D0,1.0D0), & & div(abs(t%BR_hjZZ(jj)-t%BR_HZZ_SM(jj)),t%BR_HZZ_SM(jj),0.0D0,1.0D0), & & div(abs(t%BR_hjbb(jj)-t%BR_Hbb_SM(jj)),t%BR_Hbb_SM(jj),0.0D0,1.0D0), & & div(abs(t%BR_hjtautau(jj)-t%BR_Htautau_SM(jj)),t%BR_Htautau_SM(jj),0.0D0,1.0D0) /)) if(dcbyc_dble.lt.0.1D0) then correct_properties=.True. BR_rat(1) = BR_rat(1)+t%BR_hjhihi(j,jj) endif endif enddo case(046701) ! This is a H->h(SM)h(SM) search! ns = 1; nb =1; call initialise_XS_rat_BR_rat XS_rat(1) = t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j) BR_rat(1) = 0.0D0 correct_properties=.False. do jj=1,np(Hneut) if(abs(t%particle(Hneut)%M(jj)-125.4).lt.(5.0D0+t%particle(Hneut)%dMh(jj))) then dcbyc_dble=maxval((/ div(abs(t%BR_hjgaga(jj)-t%BR_Hgaga_SM(jj)),t%BR_Hgaga_SM(jj),0.0D0,1.0D0),& & div(abs(t%BR_hjWW(jj)-t%BR_HWW_SM(jj)),t%BR_HWW_SM(jj),0.0D0,1.0D0) /)) if(dcbyc_dble.lt.0.1D0) then correct_properties=.True. BR_rat(1) = BR_rat(1)+t%BR_hjhihi(j,jj) endif endif enddo + case(8567) ! This is a H->h(SM)h(SM) search! + ns = 1; nb =1; call initialise_XS_rat_BR_rat + XS_rat(1) = t%lhc13%XS_hj_ratio(j)*t%lhc13%XS_H_SM(j) + BR_rat(1) = 0.0D0 + correct_properties=.False. + do jj=1,np(Hneut) + if(abs(t%particle(Hneut)%M(jj)-125.0).lt.(5.0D0+t%particle(Hneut)%dMh(jj))) then + dcbyc_dble=maxval((/ div(abs(t%BR_hjgaga(jj)-t%BR_Hgaga_SM(jj)),t%BR_Hgaga_SM(jj),0.0D0,1.0D0),& + & div(abs(t%BR_hjWW(jj)-t%BR_HWW_SM(jj)),t%BR_HWW_SM(jj),0.0D0,1.0D0) /)) + if(dcbyc_dble.lt.0.1D0) then + correct_properties=.True. + BR_rat(1) = BR_rat(1)+t%BR_hjhihi(j,jj) * t%BR_hjgaga(jj) * t%BR_hjWW(jj) * 2.0D0 ! symmetry factor of 2 + endif + endif + enddo + + case(4873) ! This is a H->h(SM)h(SM) search! ns = 1; nb =1; call initialise_XS_rat_BR_rat XS_rat(1) = t%lhc13%XS_hj_ratio(j)*t%lhc13%XS_H_SM(j) BR_rat(1) = 0.0D0 correct_properties=.False. do jj=1,np(Hneut) if(abs(t%particle(Hneut)%M(jj)-125.0).lt.(5.0D0+t%particle(Hneut)%dMh(jj))) then dcbyc_dble=maxval((/ div(abs(t%BR_hjgaga(jj)-t%BR_Hgaga_SM(jj)),t%BR_Hgaga_SM(jj),0.0D0,1.0D0),& & div(abs(t%BR_hjbb(jj)-t%BR_Hbb_SM(jj)),t%BR_Hbb_SM(jj),0.0D0,1.0D0) /)) if(dcbyc_dble.lt.0.1D0) then correct_properties=.True. BR_rat(1) = BR_rat(1)+t%BR_hjhihi(j,jj) endif endif enddo case(046702) ! This is a H->h(SM)h(SM) search! ns = 1; nb =1; call initialise_XS_rat_BR_rat XS_rat(1) = t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j) BR_rat(1) = 0.0D0 correct_properties=.False. do jj=1,np(Hneut) if(abs(t%particle(Hneut)%M(jj)-125.4).lt.(10.0D0+t%particle(Hneut)%dMh(jj))) then dcbyc_dble=maxval((/ div(abs(t%BR_hjbb(jj)-t%BR_Hbb_SM(jj)),t%BR_Hbb_SM(jj),0.0D0,1.0D0), & & div(abs(t%BR_hjtautau(jj)-t%BR_Htautau_SM(jj)),t%BR_Htautau_SM(jj),0.0D0,1.0D0) /)) if(dcbyc_dble.lt.0.1D0) then correct_properties=.True. BR_rat(1) = BR_rat(1)+t%BR_hjhihi(j,jj) endif endif enddo + case(336) ! This is a H->h(SM)h(SM) search! + ns = 1; nb =1; call initialise_XS_rat_BR_rat + XS_rat(1) = t%lhc13%XS_hj_ratio(j)*t%lhc13%XS_H_SM(j) + BR_rat(1) = 0.0D0 + correct_properties=.False. + do jj=1,np(Hneut) + if(abs(t%particle(Hneut)%M(jj)-125.0).lt.(10.0D0+t%particle(Hneut)%dMh(jj))) then + dcbyc_dble=maxval((/ div(abs(t%BR_hjbb(jj)-t%BR_Hbb_SM(jj)),t%BR_Hbb_SM(jj),0.0D0,1.0D0), & + & div(abs(t%BR_hjtautau(jj)-t%BR_Htautau_SM(jj)),t%BR_Htautau_SM(jj),0.0D0,1.0D0) /)) + if(dcbyc_dble.lt.0.1D0) then + correct_properties=.True. + BR_rat(1) = BR_rat(1)+t%BR_hjhihi(j,jj) * t%BR_hjbb(jj) * t%BR_hjtautau(jj) * 2.0D0 + endif + endif + enddo + + case(0038911) ! H-WW search with width-assumptions ns = 1; nb =1; call initialise_XS_rat_BR_rat XS_rat(1) = t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j) BR_rat(1) = t%BR_hjWW(j) if(t%particle(Hneut)%GammaTot(j)<0.2D0*t%GammaTot_SM(j)) then ! NWA requirement correct_properties=.True. else correct_properties=.False. endif case(0038912) ! H-WW search with width-assumptions ns = 1; nb =1; call initialise_XS_rat_BR_rat XS_rat(1) = t%lhc8%XS_vbf_ratio(j)*t%lhc8%XS_vbf_SM(j) BR_rat(1) = t%BR_hjWW(j) if(t%particle(Hneut)%GammaTot(j)<0.2D0*t%GammaTot_SM(j)) then ! NWA requirement correct_properties=.True. else correct_properties=.False. endif case(0038913) ! H-WW search with width-assumptions ns = 1; nb =1; call initialise_XS_rat_BR_rat XS_rat(1) = t%lhc8%XS_hj_ratio(j)*t%lhc8%XS_H_SM(j) BR_rat(1) = t%BR_hjWW(j) if(t%particle(Hneut)%GammaTot(j)>0.8D0*t%GammaTot_SM(j)) then ! NWA requirement correct_properties=.True. else correct_properties=.False. endif case(0038914) ! H-WW search with width-assumptions ns = 1; nb =1; call initialise_XS_rat_BR_rat XS_rat(1) = t%lhc8%XS_vbf_ratio(j)*t%lhc8%XS_vbf_SM(j) BR_rat(1) = t%BR_hjWW(j) if(t%particle(Hneut)%GammaTot(j)>0.8D0*t%GammaTot_SM(j)) then ! NWA requirement correct_properties=.True. else correct_properties=.False. endif !case(801,802,803,811,813,821) !ns = 1; nb = 1; call initialise_XS_rat_BR_rat ! XS_rat(1) = !BR_rat(1) = !if((t%BR_Hpjcb(j)+t%BR_Hpjcs(j)+t%BR_Hpjtaunu(j)).gt.0.98D0)then !else ! correct_properties=.False. !endif case default write(*,*)'hello id=',id stop 'error in subroutine model_likeness (2)' end select !---------------------------------------------------------- !--New model likeness check (TS 23/03/2012) !---------------------------------------------------------- if(allocated(channel_rat)) then if(nc.ne.ubound(channel_rat,dim=1))stop 'error in subroutine model_likeness (3a)' if(nc.ne.ubound(channel_SM,dim=1))stop 'error in subroutine model_likeness (3a)' ! Check if the channels have been filled correctly do ic=1,nc if(abs(channel_rat(ic,1)-unset).lt.1.0D-3)stop 'error in subroutine model_likeness (4a)' if(abs(channel_rat(ic,2)-unset).lt.1.0D-3)stop 'error in subroutine model_likeness (4a)' if(abs(channel_SM(ic,1)-unset).lt.1.0D-3)stop 'error in subroutine model_likeness (4a)' if(abs(channel_SM(ic,2)-unset).lt.1.0D-3)stop 'error in subroutine model_likeness (4a)' enddo !---Eliminate irrelevant channels (=channels with very small SM prediction). !---Construct mean value of the ratio for the relevant channels nc_rel=0 do ic=1,nc if(channel_SM(ic,1).gt.vsmall.and.channel_SM(ic,2).gt.vsmall) then nc_rel=nc_rel+1 channel_SM(nc_rel,:)=channel_SM(ic,:) channel_rat(nc_rel,:)=channel_rat(ic,:) endif enddo if(nc_rel.gt.0) then nc=nc_rel call reallocate_channel_rat_SM endif !--Evaluate the total SM rate expected for the (relevant) channels SMrate=0. do ic=1,nc SMrate=SMrate+channel_SM(ic,1)*channel_SM(ic,2) enddo !--Evaluate the predicted signal strength modifier c of the model c=0. do ic=1,nc !----use a weighted average of the channel rate ratios if(use_weight) then weight = div(channel_SM(ic,1)*channel_SM(ic,2),SMrate,0.0D0,1.0D9) else weight = 1.0D0/nc endif c=c+weight*channel_rat(ic,1)*channel_rat(ic,2) enddo !--Evaluate the deviation of each channel rate ratio to the signal !--strength modifier c allocate(dcbyc(nc)) do ic=1,nc dcbyc(ic)= div((channel_rat(ic,1)*channel_rat(ic,2)-c),c,0.0D0,1.0D9) enddo !--Do the model likeness test testSMratios= 1 !passes the SM-like ratios test do ic=1,nc !----Again, evaluate the weight of the channel if(use_weight) then weight = div(channel_SM(ic,1)*channel_SM(ic,2),SMrate,0.0D0,1.0D9) else weight = 1.0D0 endif !----Check if the channel fulfills the model likeness criteria ! print *, ic, channel_rat(ic,1), channel_rat(ic,2), abs(dcbyc(ic)*weight), dcbyc(ic), weight, c if(abs(dcbyc(ic)*weight).gt.eps)then testSMratios= -1 !fails the SM-like ratios test ! write(*,*) "Analysis application ", id, "fail the SM likeness test!" endif enddo !--Write total ratio into s and b to return later. s=c b=1. deallocate(channel_rat) deallocate(channel_SM) deallocate(dcbyc) !-If channel_rat is not allocated, use old method: else if(ns.ne.ubound(XS_rat,dim=1))stop 'error in subroutine model_likeness (3a)' if(nb.ne.ubound(BR_rat,dim=1))stop 'error in subroutine model_likeness (3b)' do is=1,ns if(abs(XS_rat(is)-unset).lt.1.0D-3)stop 'error in subroutine model_likeness (4a)' enddo do ib=1,nb if(abs(BR_rat(ib)-unset).lt.1.0D-3)stop 'error in subroutine model_likeness (4b)' enddo s=sum(XS_rat)/ns b=sum(BR_rat)/nb allocate(dsbys(ns)) do is=1,ns dsbys(is)= div((XS_rat(is) -s),s, 0.0D0,1.0D9) enddo allocate(dbbyb(nb)) do ib=1,nb dbbyb(ib)= div((BR_rat(ib) -b),b, 0.0D0,1.0D9) enddo testSMratios= 1 !passes the SM-like ratios test do is=1,ns do ib=1,nb if(abs( dsbys(is)+dbbyb(ib)+dsbys(is)*dbbyb(ib) ).gt.eps )then testSMratios= -1 !fails the SM-like ratios test endif enddo enddo deallocate(dsbys) deallocate(dbbyb) deallocate(XS_rat) deallocate(BR_rat) endif if(testSMratios.lt.0)correct_properties=.False. if(correct_properties)then model_like= 1 !passes the model-likeness test sigmaXbr=s*b else model_like= -1 !fails the model-likeness test sigmaXbr=0.0D0 endif contains !---------------------------------------- subroutine initialise_XS_rat_BR_rat allocate(XS_rat(ns)) allocate(BR_rat(nb)) XS_rat=unset BR_rat=unset allocate(XS_SM_temp(ns)) allocate(BR_SM_temp(nb)) XS_SM_temp=unset BR_SM_temp=unset end subroutine initialise_XS_rat_BR_rat !---------------------------------------- subroutine initialise_channel_rat_SM allocate(channel_rat(nc,2)) allocate(channel_SM(nc,2)) channel_rat=unset channel_SM=unset end subroutine initialise_channel_rat_SM !---------------------------------------- subroutine reallocate_channel_rat_SM double precision, allocatable :: reallocate_array(:,:) allocate(reallocate_array(nc,2)) reallocate_array(1:nc,:) = channel_rat(1:nc,:) deallocate(channel_rat) allocate(channel_rat(nc,2)) channel_rat = reallocate_array reallocate_array(1:nc,:) = channel_SM(1:nc,:) deallocate(channel_SM) allocate(channel_SM(nc,2)) channel_SM = reallocate_array deallocate(reallocate_array) end subroutine reallocate_channel_rat_SM !---------------------------------------- end subroutine model_likeness !*********************************************************** subroutine fill_blank_ft1_dat(ft1,ft1_sep,vmasslower,vmasshigher,vmass_xmin,vmass_xmax,vmass_sep,valueoutsidetable) ! don't forget to deallocate f_t1%dat use usefulbits, only : small implicit none integer :: ilower,ihigher double precision, intent(in) :: ft1_sep,vmasslower,vmasshigher,vmass_xmin,vmass_xmax,vmass_sep,valueoutsidetable type(table1) :: ft1 if(abs(vmass_xmin-vmass_xmax).lt.small)stop 'problem in f_from_t3 (4)' ft1%sep=ft1_sep ! we want f_t1%xmin to be lower than x1lower if((vmasslower -vmass_xmin).ge.0.0D0)then ilower = int((vmasslower -vmass_xmin)/vmass_sep)+1 else !off lower edge of table ilower = int((vmasslower -vmass_xmin)/vmass_sep)+1-1 !-1 since int rounds up for negative numbers endif ihigher = int((vmasshigher-vmass_xmin)/vmass_sep)+2 ! we want f_t1%xmax to be higher than x1higher ft1%xmin = dble(ilower - 1)*vmass_sep + vmass_xmin ft1%xmax = dble(ihigher - 1)*vmass_sep + vmass_xmin ft1%nx=nint((ft1%xmax-ft1%xmin)/ft1%sep)+1 allocate(ft1%dat(ft1%nx,1)) ft1%dat(:,1)=valueoutsidetable end subroutine fill_blank_ft1_dat !*********************************************************** subroutine f_from_t1(t1,vmasslower,vmasshigher,sepmultfactor,datcomp, & & f_t1,valueoutsidetable) ! Fills the f_t1 array with the information from a t1 array ! ! Do not forget to deallocate f_t1%dat later on !*********************************************************** use interpolate use usefulbits, only : small implicit none !--------------------------------------input type(table1), intent(in) :: t1 double precision, intent(in) :: vmasslower,vmasshigher,valueoutsidetable double precision, intent(in) :: sepmultfactor integer, intent(in) :: datcomp !-----------------------------------output type(table1), intent(out) :: f_t1 !-----------------------------------internal integer :: i double precision :: interpol double precision :: vmass,vmass_xmin,vmass_xmax,vmass_sep !------------------------------------------- if(vmasslower.gt.vmasshigher)then stop 'problem in f_from_t1 (1)' endif f_t1%id = t1%id f_t1%deltax = t1%deltax vmass_xmin = t1%xmin vmass_xmax = t1%xmax vmass_sep = t1%sep f_t1%sep = t1%sep*sepmultfactor call fill_blank_ft1_dat(f_t1,f_t1%sep,vmasslower,vmasshigher,vmass_xmin,vmass_xmax,vmass_sep,valueoutsidetable) do i=1,ubound(f_t1%dat,dim=1) vmass = dble(i-1)*f_t1%sep + f_t1%xmin if( vmass.lt.vmass_xmin-small )then f_t1%dat(i,1)=valueoutsidetable elseif( vmass.gt.vmass_xmax+small )then f_t1%dat(i,1)=valueoutsidetable else call interpolate_tabletype1(vmass,t1,datcomp,interpol) f_t1%dat(i,1)=interpol endif enddo end subroutine f_from_t1 !*********************************************************** subroutine f_from_t2(t2,m1_at_ref_point_1,m2_at_ref_point_1,m1_at_ref_point_2,m2_at_ref_point_2, & & vmassm1orm2,vmasslower,vmasshigher,sepmultfactor,datcomp, & & f_t1,valueoutsidetable) ! Fills the f_t1 array with the information from a t2 array along a line ! m2 = line_grad*m1 + line_const ! ! Do not forget to deallocate f_t1%dat later on !*********************************************************** use interpolate use usefulbits, only : small implicit none !--------------------------------------input type(table2), intent(in) :: t2 double precision, intent(in) :: m1_at_ref_point_1,m2_at_ref_point_1,m1_at_ref_point_2,m2_at_ref_point_2 double precision, intent(in) :: vmasslower,vmasshigher,valueoutsidetable double precision, intent(in) :: sepmultfactor integer, intent(in) :: datcomp,vmassm1orm2 !-----------------------------------output type(table1), intent(out) :: f_t1 !-----------------------------------internal type(table1) :: t1 double precision :: line_grad,line_const integer :: i logical :: const_m1,const_m2 integer :: const_m1_i,const_m2_j logical :: on_m1_gridline,on_m2_gridline double precision :: interpol,mass1,mass2 double precision :: m1bit,m2bit double precision :: vmass,vmass_xmin,vmass_xmax,vmass_sep integer :: ftype_selection(1) !------------------------------------------- if(vmasslower.gt.vmasshigher)then stop 'problem in f_from_t2 (1)' endif if(abs(m1_at_ref_point_1-m1_at_ref_point_2).lt.small)then const_m1=.True. !line_grad is not needed !line_const is not needed else const_m1=.False. line_grad =(m2_at_ref_point_1-m2_at_ref_point_2)/(m1_at_ref_point_1-m1_at_ref_point_2) line_const=(m1_at_ref_point_1*m2_at_ref_point_2-m1_at_ref_point_2*m2_at_ref_point_1) & & /(m1_at_ref_point_1-m1_at_ref_point_2) endif if(abs(m2_at_ref_point_1-m2_at_ref_point_2).lt.small)then const_m2=.True. else const_m2=.False. endif f_t1%id = t2%id f_t1%deltax = t2%deltax select case(vmassm1orm2) case(1) if(const_m1)stop 'problem in f_from_t2 (3a)' vmass_xmin = t2%xmin1 vmass_xmax = t2%xmax1 vmass_sep = t2%sep1 f_t1%sep = t2%sep1*sepmultfactor case(2) if(const_m2)stop 'problem in f_from_t2 (3b)' vmass_xmin = t2%xmin2 vmass_xmax = t2%xmax2 vmass_sep = t2%sep2 f_t1%sep = t2%sep2*sepmultfactor case default stop 'problem in f_from_t2 (3)' end select call fill_blank_ft1_dat(f_t1,f_t1%sep,vmasslower,vmasshigher,vmass_xmin,vmass_xmax,vmass_sep,valueoutsidetable) on_m1_gridline=.False. if(const_m1)then const_m1_i=nint( (m1_at_ref_point_1-t2%xmin1) /t2%sep1)+1 m1bit= m1_at_ref_point_1 -(dble(const_m1_i-1)*t2%sep1+t2%xmin1)/t2%sep1 if(m1bit.lt.small)on_m1_gridline=.True. endif on_m2_gridline=.False. if(const_m2)then const_m2_j=nint( (m2_at_ref_point_1-t2%xmin2) /t2%sep2)+1 m2bit= m2_at_ref_point_1 -(dble(const_m2_j-1)*t2%sep2+t2%xmin2)/t2%sep2 if(m2bit.lt.small)on_m2_gridline=.True. endif ftype_selection(1)=datcomp if( on_m1_gridline )then call fill_t1_from_t2(t2,2,const_m1_i,ftype_selection,t1) call f_from_t1(t1,vmasslower,vmasshigher,sepmultfactor,datcomp, & & f_t1,valueoutsidetable) deallocate(t1%dat) elseif(on_m2_gridline )then call fill_t1_from_t2(t2,1,const_m2_j,ftype_selection,t1) call f_from_t1(t1,vmasslower,vmasshigher,sepmultfactor,datcomp, & & f_t1,valueoutsidetable) deallocate(t1%dat) else do i=1,ubound(f_t1%dat,dim=1) vmass = dble(i-1)*f_t1%sep + f_t1%xmin if(t2%nx2.eq.1)then mass1 = vmass mass2 = t2%xmin2 elseif(vmassm1orm2.eq.1)then mass1 = vmass mass2 = mass1*line_grad+line_const else mass2 = vmass if(const_m1)then mass1 = m1_at_ref_point_1 else mass1 = (mass2 - line_const)/line_grad endif endif if( vmass.lt.vmass_xmin-small )then f_t1%dat(i,1)=valueoutsidetable elseif( vmass.gt.vmass_xmax+small )then f_t1%dat(i,1)=valueoutsidetable elseif(( t2%needs_M2_gt_2M1 ).and.(2.0D0*mass1>mass2+small))then f_t1%dat(i,1)=valueoutsidetable elseif((.not.(t2%needs_M2_gt_2M1)).and.(mass1>mass2+small).and.(t2%nx2.gt.1))then f_t1%dat(i,1)=valueoutsidetable else call interpolate_tabletype2(mass1,mass2,t2,datcomp,interpol) f_t1%dat(i,1)=interpol endif enddo endif end subroutine f_from_t2 !****************************************************************** subroutine f_from_slices_t2(slices_t2,m1_at_ref_point_1,m2_at_ref_point_1,m1_at_ref_point_2,m2_at_ref_point_2,z, & & vmassm1orm2,vmasslower,vmasshigher,sepmultfactor,datcomp, & & f_t1,valueoutsidetable) !****************************************************************** ! fill the f_t1 array with the information from a t3 array at constant sf along a line ! m2 = line_grad*m1 + line_const ! do not forget to deallocate dat use S95tables_type3 use interpolate use usefulbits, only : small implicit none type(table2), intent(in) :: slices_t2(2) type(table1) :: f_t1 double precision, intent(in) :: m1_at_ref_point_1,m2_at_ref_point_1,m1_at_ref_point_2,m2_at_ref_point_2 double precision, intent(in) :: z,vmasslower,vmasshigher,valueoutsidetable double precision, intent(in) :: sepmultfactor double precision :: line_grad,line_const integer, intent(in) :: datcomp,vmassm1orm2 integer :: i logical :: const_m1,const_m2 double precision :: interpol,mass1,mass2 double precision :: vmass,vmass_xmin,vmass_xmax,vmass_sep double precision :: z_below,z_above if(vmasslower.gt.vmasshigher)then stop 'problem in f_from_slices_t2 (1)' endif if(abs(m1_at_ref_point_1-m1_at_ref_point_2).lt.small)then const_m1=.True. else const_m1=.False. endif if(abs(m2_at_ref_point_1-m2_at_ref_point_2).lt.small)then const_m2=.True. else const_m2=.False. endif ! check if mass is within z range of table: if( .not. ( (z .ge. slices_t2(1)%z-small).and.(z .le. slices_t2(2)%z+small) ) )then !#1! written in convoluted way to get the NaNs f_t1%id = slices_t2(1)%id f_t1%deltax = slices_t2(1)%deltax if((slices_t2(1)%nx2.eq.1).or.(vmassm1orm2.eq.1))then if(const_m1)stop 'problem in f_from_slices_t2 (1a)' vmass_xmin = slices_t2(1)%xmin1 vmass_sep = slices_t2(1)%sep1 f_t1%sep = slices_t2(1)%sep1*sepmultfactor else if(const_m2)stop 'problem in f_from_slices_t2 (1b)' vmass_xmin = slices_t2(1)%xmin2 vmass_sep = slices_t2(1)%sep2 f_t1%sep = slices_t2(1)%sep2*sepmultfactor endif call fill_blank_ft1_dat(f_t1,f_t1%sep,vmasslower,vmasshigher,vmass_xmin,vmass_xmax,vmass_sep,valueoutsidetable) else !#1 z_below=slices_t2(1)%z z_above=slices_t2(2)%z if(abs(z_below-z).lt.small)then !z is the same as z_below !#2 call f_from_t2(slices_t2(1),m1_at_ref_point_1,m2_at_ref_point_1,m1_at_ref_point_2,m2_at_ref_point_2, & & vmassm1orm2,vmasslower,vmasshigher,sepmultfactor,1, & & f_t1,valueoutsidetable) elseif(abs(z_above-z).lt.small)then !z is the same as z_above !#2 call f_from_t2(slices_t2(2),m1_at_ref_point_1,m2_at_ref_point_1,m1_at_ref_point_2,m2_at_ref_point_2, & & vmassm1orm2,vmasslower,vmasshigher,sepmultfactor,1, & & f_t1,valueoutsidetable) else!#2 if(const_m1)then !line_grad is not needed !line_const is not needed else line_grad =(m2_at_ref_point_1-m2_at_ref_point_2)/(m1_at_ref_point_1-m1_at_ref_point_2) line_const=(m1_at_ref_point_1*m2_at_ref_point_2-m1_at_ref_point_2*m2_at_ref_point_1) & & /(m1_at_ref_point_1-m1_at_ref_point_2) endif f_t1%id = slices_t2(1)%id f_t1%deltax = slices_t2(1)%deltax if((slices_t2(1)%nx2.eq.1).or.(vmassm1orm2.eq.1))then vmass_xmin = slices_t2(1)%xmin1 vmass_xmax = slices_t2(1)%xmax1 vmass_sep = slices_t2(1)%sep1 f_t1%sep = slices_t2(1)%sep1*sepmultfactor else if(const_m2)stop 'problem in f_from_slices_t2 (3b)' vmass_xmin = slices_t2(1)%xmin2 vmass_xmax = slices_t2(1)%xmax2 vmass_sep = slices_t2(1)%sep2 f_t1%sep = slices_t2(1)%sep2*sepmultfactor endif call fill_blank_ft1_dat(f_t1,f_t1%sep,vmasslower,vmasshigher,vmass_xmin,vmass_xmax,vmass_sep,valueoutsidetable) do i=1,ubound(f_t1%dat,dim=1) vmass = dble(i-1)*f_t1%sep + f_t1%xmin if(slices_t2(1)%nx2.eq.1)then mass1 = vmass mass2 = slices_t2(1)%xmin2 else select case(vmassm1orm2) case(1) mass1 = vmass mass2 = mass1*line_grad+line_const case(2) mass2 = vmass if(const_m1)then mass1 = m1_at_ref_point_1 else mass1 = (mass2 - line_const)/line_grad endif case default stop 'problem in f_from_slices_t2 (4b)' end select endif if( vmass.lt.vmass_xmin-small )then f_t1%dat(i,1)=valueoutsidetable elseif( vmass.gt.vmass_xmax+small )then f_t1%dat(i,1)=valueoutsidetable elseif((slices_t2(1)%nx2.gt.1).and.( slices_t2(1)%needs_M2_gt_2M1 ).and.(2.0D0*mass1>mass2+small))then f_t1%dat(i,1)=valueoutsidetable elseif((slices_t2(1)%nx2.gt.1).and.(.not.(slices_t2(1)%needs_M2_gt_2M1)).and.(mass1>mass2+small))then f_t1%dat(i,1)=valueoutsidetable else call interpolate_slices_t2(mass1,mass2,z,slices_t2,datcomp,interpol) f_t1%dat(i,1)=interpol endif enddo endif !#2 endif !#1 end subroutine f_from_slices_t2 !****************************************************************** subroutine f_from_t3(t3,m1_at_ref_point_1,m2_at_ref_point_1,m1_at_ref_point_2,m2_at_ref_point_2,z, & & vmassm1orm2,vmasslower,vmasshigher,sepmultfactor,datcomp, & & f_t1,valueoutsidetable) !****************************************************************** ! fill the f_t1 array with the information from a t3 array at constant sf along a line ! m2 = line_grad*m1 + line_const ! do not forget to deallocate dat use S95tables_type3 use interpolate use usefulbits, only : small implicit none type(table3), intent(in) :: t3 type(table2) :: slices_t2(2) type(table1) :: f_t1 double precision, intent(in) :: m1_at_ref_point_1,m2_at_ref_point_1,m1_at_ref_point_2,m2_at_ref_point_2 double precision, intent(in) :: z,vmasslower,vmasshigher,valueoutsidetable double precision, intent(in) :: sepmultfactor integer, intent(in) :: datcomp,vmassm1orm2 integer :: a logical :: const_m1,const_m2 double precision :: vmass_xmin,vmass_xmax,vmass_sep integer :: ilow,c_zi(2),ftype_selection(1) double precision :: z_below,z_above if(vmasslower.gt.vmasshigher)then stop 'problem in f_from_t3 (1)' endif if(abs(m1_at_ref_point_1-m1_at_ref_point_2).lt.small)then const_m1=.True. else const_m1=.False. endif if(abs(m2_at_ref_point_1-m2_at_ref_point_2).lt.small)then const_m2=.True. else const_m2=.False. endif ! check if mass is within z range of table: if( .not. ( (z .ge. t3%zmin-small).and.(z .le. t3%zmax+small) ) )then !#1! written in convoluted way to get the NaNs f_t1%id = t3%id f_t1%deltax = t3%deltax if((t3%nx2.eq.1).or.(vmassm1orm2.eq.1))then if(const_m1)stop 'problem in f_from_t3 (1a)' vmass_xmin = t3%xmin1 vmass_sep = t3%sep1 f_t1%sep = t3%sep1*sepmultfactor else if(const_m2)stop 'problem in f_from_t3 (1b)' vmass_xmin = t3%xmin2 vmass_sep = t3%sep2 f_t1%sep = t3%sep2*sepmultfactor endif call fill_blank_ft1_dat(f_t1,f_t1%sep,vmasslower,vmasshigher,vmass_xmin,vmass_xmax,vmass_sep,valueoutsidetable) else !#1 ilow=int((z-t3%zmin)/t3%zsep)+1 z_below=dble(ilow-1)*t3%zsep+t3%zmin z_above=z_below+t3%zsep if(abs(z_below-z).lt.small)then !z is the same as z_below !#2 c_zi= ilow elseif(abs(z_above-z).lt.small)then !z is the same as z_above !#2 c_zi= ilow+1 else !#2 c_zi(1)= ilow c_zi(2)= ilow+1 endif !#2 ftype_selection(1)=datcomp call fill_slices_t2_from_slices_of_t3(t3,c_zi,ftype_selection,slices_t2) call f_from_slices_t2(slices_t2,m1_at_ref_point_1,m2_at_ref_point_1,m1_at_ref_point_2,m2_at_ref_point_2,z, & & vmassm1orm2,vmasslower,vmasshigher,sepmultfactor,datcomp, & & f_t1,valueoutsidetable) do a=1,2 deallocate(slices_t2(a)%dat) enddo endif !#1 end subroutine f_from_t3 !************************************************************ subroutine convolve_chisq_with_gaussian(t1,datcomp,sigma,mass,result) !************************************************************ ! intergrate exp(-t1%dat(xi,1)/2)*exp(-(massx-mass)^2/(2*sigma^2))/sqrt(2*pi*sigma^2) w.r.t. x ! between xlower and xhigher ! then do -2.0D0*log to get result ! negative data points are invalid. They are set to zero. use usefulbits, only : vsmall,vvsmall,pi !internal use interpolate use S95tables_type1 implicit none type(table1),intent(in) :: t1 integer,intent(in) :: datcomp double precision,intent(in) :: sigma,mass double precision,intent(out) :: result !-----------------------------------internal integer :: i,ilow,ihigh,j,divisions,n,ntot double precision :: runningtotal,massx,datvalue,newsep double precision,allocatable :: newdat(:) double precision :: big_number_instead_of_infinity double precision :: dati,datiplus1 !------------------------------------------- if((datcomp.lt.lbound(t1%dat,dim=2)).or.(datcomp.gt.ubound(t1%dat,dim=2)))then stop 'wrong datcomp inputted to subroutine convolve_with_gaussian' elseif(t1%nx.le.1)then stop 'wrong t1%nx inputted to subroutine convolve_with_gaussian (2)' elseif(sigma.le.vsmall)then stop 'wrong sigma inputted to subroutine convolve_with_gaussian' elseif(abs(t1%sep).le.vsmall)then stop 'wrong t1%sep inputted to subroutine convolve_with_gaussian' endif big_number_instead_of_infinity=1.0D5 divisions=5 !do i=1,t1%nx ! if(t1%dat(i,datcomp).ge.big_number_instead_of_infinity)t1%dat(i,datcomp)=1.0D20 !enddo n=0 if(minval(t1%dat(:,datcomp)).lt.1.0D4)then ilow = lbound(t1%dat,dim=1) ihigh = ubound(t1%dat,dim=1) if(ilow.eq.ihigh)stop 'problem in subroutine convolve_with_gaussian' newsep=t1%sep/dble(divisions) ntot=divisions*(ihigh-ilow)+1 allocate(newdat(ntot)) newdat=0.0D0 do i=ilow,ihigh dati=t1%dat(i,datcomp) if(dati.ge.0.0D0)then n=n+1 massx=dble(i-1)*t1%sep+t1%xmin datvalue=dati newdat(n)=exp(-datvalue/2.0D0) & & *exp(-(massx-mass)**2.0D0/(2.0D0*sigma**2.0D0))/sqrt(2.0D0*pi*sigma**2.0D0) if(i.lt.ihigh)then datiplus1=t1%dat(i+1,datcomp) if(datiplus1.ge.0.0D0)then do j=2,divisions-1 n=n+1 massx=dble(i-1)*t1%sep+t1%xmin + dble(j-1)*newsep !do a=1,ihigh ! write(*,*)a,dble(a-1)*t1%sep+t1%xmin ,t1%dat(a,datcomp) !enddo datvalue=dati +((datiplus1-dati)/t1%sep)*dble(j-1)*newsep if(datvalue.lt.0.0D0)then !these are invalid point or places outside range of table datvalue=0.0D0 endif newdat(n)=exp(-datvalue/2.0D0) & & *exp(-(massx-mass)**2.0D0/(2.0D0*sigma**2.0D0))/sqrt(2.0D0*pi*sigma**2.0D0) enddo else do j=2,divisions-1 n=n+1 enddo endif else !negative data points are invalid do j=2,divisions-1 n=n+1 enddo endif !massx=dble(i-1)*t1%sep+t1%xmin !newdat(i)=exp(-t1%dat(i,datcomp)/2.0D0) & ! & *exp(-(massx-mass)**2.0D0/(2.0D0*sigma**2.0D0))/sqrt(2.0D0*pi*sigma**2.0D0) else do j=1,divisions-1 n=n+1 enddo endif enddo !intergrate with trapezium rule runningtotal=0.5D0*(newdat(1)+newdat(ntot)) if((ntot).gt.1)then do n=2,ntot-1 runningtotal=runningtotal+newdat(n) enddo endif deallocate(newdat) if(abs(runningtotal).le.vvsmall)then result= big_number_instead_of_infinity else result= -2.0D0*log(runningtotal*newsep) endif if(result.gt.22.4D0)then !corresponds to clsb=1.0D-6, which is the lowest clsb that ppchi2 can take as input result= big_number_instead_of_infinity endif else result= big_number_instead_of_infinity endif end subroutine convolve_chisq_with_gaussian !************************************************************ function S95_t1_or_S95_t2_idfromelementnumber(ttype,tlist) !************************************************************ implicit none integer :: S95_t1_or_S95_t2_idfromelementnumber integer,intent(in) ::tlist integer,intent(in) ::ttype select case(ttype) case(1) S95_t1_or_S95_t2_idfromelementnumber=S95_t1(tlist)%id case(2) S95_t1_or_S95_t2_idfromelementnumber=S95_t2(tlist)%id case(9) S95_t1_or_S95_t2_idfromelementnumber=3316 case default stop 'wrong input to function S95_t1_or_S95_t2_idfromelementnumber' end select end function S95_t1_or_S95_t2_idfromelementnumber !************************************************************ function S95_t1_or_S95_t2_elementnumberfromid(ttype,id) !************************************************************ use S95tables_type1, only :t1elementnumberfromid use S95tables_type2, only :t2elementnumberfromid implicit none integer,intent(in) ::id integer,intent(in) ::ttype integer :: S95_t1_or_S95_t2_elementnumberfromid select case(ttype) case(1) S95_t1_or_S95_t2_elementnumberfromid= t1elementnumberfromid(S95_t1,id) case(2) S95_t1_or_S95_t2_elementnumberfromid= t2elementnumberfromid(S95_t2,id) case default stop 'problem with function S95_t1_or_S95_t2_elementnumberfromid' end select end function S95_t1_or_S95_t2_elementnumberfromid !************************************************************ subroutine deallocate_S95tables !************************************************************ implicit none !-----------------------------------internal integer x !------------------------------------------- do x=lbound(S95_t1,dim=1),ubound(S95_t1,dim=1) deallocate(S95_t1(x)%dat) enddo do x=lbound(S95_t2,dim=1),ubound(S95_t2,dim=1) deallocate(S95_t2(x)%dat) enddo deallocate(S95_t1) deallocate(S95_t2) call deallocate_Exptranges end subroutine deallocate_S95tables !*********************************************************** subroutine deallocate_Exptranges !*********************************************************** implicit none if(allocated(Exptrange_Mhmin_forSMXS)) deallocate(Exptrange_Mhmin_forSMXS) if(allocated(Exptrange_Mhmax_forSMXS)) deallocate(Exptrange_Mhmax_forSMXS) if(allocated(Exptrange_Mhmin_forSMdecays)) deallocate(Exptrange_Mhmin_forSMdecays) if(allocated(Exptrange_Mhmax_forSMdecays)) deallocate(Exptrange_Mhmax_forSMdecays) end subroutine deallocate_Exptranges !*********************************************************** end module S95tables !************************************************************ Index: trunk/HiggsBounds-5/Expt_tables/ATLtables/6682_Atlas_VBF_h-invisible_13TeV_36.1fb-1.txt =================================================================== --- trunk/HiggsBounds-5/Expt_tables/ATLtables/6682_Atlas_VBF_h-invisible_13TeV_36.1fb-1.txt (revision 0) +++ trunk/HiggsBounds-5/Expt_tables/ATLtables/6682_Atlas_VBF_h-invisible_13TeV_36.1fb-1.txt (revision 587) @@ -0,0 +1,591 @@ +# ATLAS, arXiv:1809.06682, Sept. 2018, Fig. 6b +# 6682_Atlas_VBF_h-invisible_13TeV_36.1fb-1.txt +# Limit set on sigma(h,VBF) x BR(h->inv) in pb +# Mh obs exp + + 75.00 1.979 1.502 + 80.00 1.942 1.473 + 85.00 1.905 1.444 + 90.00 1.867 1.414 + 95.00 1.830 1.385 + 100.0 1.793 1.356 + 105.0 1.756 1.327 + 110.0 1.719 1.298 + 115.0 1.681 1.269 + 120.0 1.644 1.240 + 125.0 1.607 1.211 + 130.0 1.586 1.195 + 135.0 1.565 1.180 + 140.0 1.544 1.165 + 145.0 1.523 1.149 + 150.0 1.502 1.134 + 155.0 1.481 1.118 + 160.0 1.460 1.103 + 165.0 1.439 1.088 + 170.0 1.418 1.072 + 175.0 1.397 1.057 + 180.0 1.377 1.042 + 185.0 1.356 1.026 + 190.0 1.335 1.011 + 195.0 1.314 0.9958 + 200.0 1.293 0.9805 + 205.0 1.272 0.9651 + 210.0 1.251 0.9498 + 215.0 1.230 0.9344 + 220.0 1.209 0.9191 + 225.0 1.188 0.9038 + 230.0 1.167 0.8884 + 235.0 1.146 0.8731 + 240.0 1.125 0.8577 + 245.0 1.104 0.8424 + 250.0 1.083 0.8271 + 255.0 1.062 0.8117 + 260.0 1.041 0.7964 + 265.0 1.020 0.7811 + 270.0 0.9994 0.7657 + 275.0 0.9784 0.7504 + 280.0 0.9575 0.7350 + 285.0 0.9365 0.7197 + 290.0 0.9156 0.7044 + 295.0 0.8946 0.6890 + 300.0 0.8737 0.6737 + 305.0 0.8694 0.6704 + 310.0 0.8650 0.6671 + 315.0 0.8607 0.6639 + 320.0 0.8564 0.6606 + 325.0 0.8520 0.6573 + 330.0 0.8477 0.6540 + 335.0 0.8434 0.6508 + 340.0 0.8391 0.6475 + 345.0 0.8347 0.6442 + 350.0 0.8304 0.6409 + 355.0 0.8261 0.6377 + 360.0 0.8218 0.6344 + 365.0 0.8174 0.6311 + 370.0 0.8131 0.6278 + 375.0 0.8088 0.6246 + 380.0 0.8044 0.6213 + 385.0 0.8001 0.6180 + 390.0 0.7958 0.6147 + 395.0 0.7915 0.6115 + 400.0 0.7871 0.6082 + 405.0 0.7828 0.6049 + 410.0 0.7785 0.6016 + 415.0 0.7742 0.5984 + 420.0 0.7698 0.5951 + 425.0 0.7655 0.5918 + 430.0 0.7612 0.5885 + 435.0 0.7568 0.5853 + 440.0 0.7525 0.5820 + 445.0 0.7482 0.5787 + 450.0 0.7439 0.5754 + 455.0 0.7395 0.5722 + 460.0 0.7352 0.5689 + 465.0 0.7309 0.5656 + 470.0 0.7265 0.5623 + 475.0 0.7222 0.5591 + 480.0 0.7179 0.5558 + 485.0 0.7136 0.5525 + 490.0 0.7092 0.5492 + 495.0 0.7049 0.5460 + 500.0 0.7006 0.5427 + 505.0 0.6963 0.5394 + 510.0 0.6919 0.5361 + 515.0 0.6876 0.5329 + 520.0 0.6833 0.5296 + 525.0 0.6789 0.5263 + 530.0 0.6746 0.5230 + 535.0 0.6703 0.5198 + 540.0 0.6660 0.5165 + 545.0 0.6616 0.5132 + 550.0 0.6573 0.5099 + 555.0 0.6530 0.5067 + 560.0 0.6487 0.5034 + 565.0 0.6443 0.5001 + 570.0 0.6400 0.4968 + 575.0 0.6357 0.4936 + 580.0 0.6313 0.4903 + 585.0 0.6270 0.4870 + 590.0 0.6227 0.4837 + 595.0 0.6184 0.4805 + 600.0 0.6140 0.4772 + 605.0 0.6097 0.4739 + 610.0 0.6054 0.4706 + 615.0 0.6011 0.4674 + 620.0 0.5967 0.4641 + 625.0 0.5924 0.4608 + 630.0 0.5881 0.4575 + 635.0 0.5837 0.4543 + 640.0 0.5794 0.4510 + 645.0 0.5751 0.4477 + 650.0 0.5708 0.4444 + 655.0 0.5664 0.4412 + 660.0 0.5621 0.4379 + 665.0 0.5578 0.4346 + 670.0 0.5535 0.4313 + 675.0 0.5491 0.4281 + 680.0 0.5448 0.4248 + 685.0 0.5405 0.4215 + 690.0 0.5361 0.4182 + 695.0 0.5318 0.4150 + 700.0 0.5275 0.4117 + 705.0 0.5232 0.4084 + 710.0 0.5188 0.4051 + 715.0 0.5145 0.4019 + 720.0 0.5102 0.3986 + 725.0 0.5058 0.3953 + 730.0 0.5015 0.3920 + 735.0 0.4972 0.3888 + 740.0 0.4929 0.3855 + 745.0 0.4885 0.3822 + 750.0 0.4842 0.3789 + 755.0 0.4827 0.3779 + 760.0 0.4813 0.3768 + 765.0 0.4798 0.3758 + 770.0 0.4783 0.3747 + 775.0 0.4768 0.3737 + 780.0 0.4754 0.3726 + 785.0 0.4739 0.3716 + 790.0 0.4724 0.3705 + 795.0 0.4709 0.3695 + 800.0 0.4695 0.3684 + 805.0 0.4680 0.3674 + 810.0 0.4665 0.3663 + 815.0 0.4651 0.3653 + 820.0 0.4636 0.3642 + 825.0 0.4621 0.3632 + 830.0 0.4606 0.3621 + 835.0 0.4592 0.3611 + 840.0 0.4577 0.3600 + 845.0 0.4562 0.3589 + 850.0 0.4547 0.3579 + 855.0 0.4533 0.3568 + 860.0 0.4518 0.3558 + 865.0 0.4503 0.3547 + 870.0 0.4488 0.3537 + 875.0 0.4474 0.3526 + 880.0 0.4459 0.3516 + 885.0 0.4444 0.3505 + 890.0 0.4429 0.3495 + 895.0 0.4415 0.3484 + 900.0 0.4400 0.3474 + 905.0 0.4385 0.3463 + 910.0 0.4371 0.3453 + 915.0 0.4356 0.3442 + 920.0 0.4341 0.3432 + 925.0 0.4326 0.3421 + 930.0 0.4312 0.3411 + 935.0 0.4297 0.3400 + 940.0 0.4282 0.3389 + 945.0 0.4267 0.3379 + 950.0 0.4253 0.3368 + 955.0 0.4238 0.3358 + 960.0 0.4223 0.3347 + 965.0 0.4208 0.3337 + 970.0 0.4194 0.3326 + 975.0 0.4179 0.3316 + 980.0 0.4164 0.3305 + 985.0 0.4149 0.3295 + 990.0 0.4135 0.3284 + 995.0 0.4120 0.3274 + 1000. 0.4105 0.3263 + 1005. 0.4102 0.3261 + 1010. 0.4098 0.3258 + 1015. 0.4094 0.3255 + 1020. 0.4091 0.3253 + 1025. 0.4087 0.3250 + 1030. 0.4083 0.3247 + 1035. 0.4079 0.3245 + 1040. 0.4076 0.3242 + 1045. 0.4072 0.3239 + 1050. 0.4068 0.3237 + 1055. 0.4065 0.3234 + 1060. 0.4061 0.3232 + 1065. 0.4057 0.3229 + 1070. 0.4054 0.3226 + 1075. 0.4050 0.3224 + 1080. 0.4046 0.3221 + 1085. 0.4043 0.3218 + 1090. 0.4039 0.3216 + 1095. 0.4035 0.3213 + 1100. 0.4032 0.3211 + 1105. 0.4028 0.3208 + 1110. 0.4024 0.3205 + 1115. 0.4021 0.3203 + 1120. 0.4017 0.3200 + 1125. 0.4013 0.3197 + 1130. 0.4009 0.3195 + 1135. 0.4006 0.3192 + 1140. 0.4002 0.3189 + 1145. 0.3998 0.3187 + 1150. 0.3995 0.3184 + 1155. 0.3991 0.3182 + 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0.3499 0.2815 + 2750. 0.3500 0.2816 + 2755. 0.3501 0.2816 + 2760. 0.3502 0.2817 + 2765. 0.3503 0.2817 + 2770. 0.3504 0.2818 + 2775. 0.3504 0.2818 + 2780. 0.3505 0.2819 + 2785. 0.3506 0.2819 + 2790. 0.3507 0.2820 + 2795. 0.3508 0.2821 + 2800. 0.3509 0.2821 + 2805. 0.3510 0.2822 + 2810. 0.3511 0.2822 + 2815. 0.3511 0.2823 + 2820. 0.3512 0.2823 + 2825. 0.3513 0.2824 + 2830. 0.3514 0.2824 + 2835. 0.3515 0.2825 + 2840. 0.3516 0.2825 + 2845. 0.3517 0.2826 + 2850. 0.3518 0.2826 + 2855. 0.3518 0.2827 + 2860. 0.3519 0.2827 + 2865. 0.3520 0.2828 + 2870. 0.3521 0.2828 + 2875. 0.3522 0.2829 + 2880. 0.3523 0.2829 + 2885. 0.3524 0.2830 + 2890. 0.3525 0.2831 + 2895. 0.3525 0.2831 + 2900. 0.3526 0.2832 + 2905. 0.3527 0.2832 + 2910. 0.3528 0.2833 + 2915. 0.3529 0.2833 + 2920. 0.3530 0.2834 + 2925. 0.3531 0.2834 + 2930. 0.3532 0.2835 + 2935. 0.3532 0.2835 + 2940. 0.3533 0.2836 + 2945. 0.3534 0.2836 + 2950. 0.3535 0.2837 + 2955. 0.3536 0.2837 + 2960. 0.3537 0.2838 + 2965. 0.3538 0.2838 + 2970. 0.3539 0.2839 + 2975. 0.3539 0.2839 + 2980. 0.3540 0.2840 + 2985. 0.3541 0.2841 + 2990. 0.3542 0.2841 + 2995. 0.3543 0.2842 + 3000. 0.3544 0.2842 Index: trunk/HiggsBounds-5/Expt_tables/ATLtables/2018025_Atlas_h-gaga_13TeV_80fb-1.txt =================================================================== --- trunk/HiggsBounds-5/Expt_tables/ATLtables/2018025_Atlas_h-gaga_13TeV_80fb-1.txt (revision 0) +++ trunk/HiggsBounds-5/Expt_tables/ATLtables/2018025_Atlas_h-gaga_13TeV_80fb-1.txt (revision 587) @@ -0,0 +1,456 @@ +# ATLAS-CONF-2018-025, 4 July 2017 +# 2018025_Atlas_h-gaga_13TeV_80fb-1 +# read in from Fig. 4b. FIDUCIAL CROSS SECTION in fb! +# Mh observed expected + + 65.00 88.70 72.39 + 65.10 89.76 72.00 + 65.20 90.83 71.61 + 65.30 91.89 71.22 + 65.40 92.96 70.83 + 65.50 94.02 70.43 + 65.60 95.09 70.04 + 65.70 96.15 69.65 + 65.80 97.22 69.26 + 65.90 98.28 68.87 + 66.00 99.35 68.48 + 66.10 99.61 68.28 + 66.20 99.87 68.09 + 66.30 100.1 67.89 + 66.40 100.4 67.70 + 66.50 100.7 67.50 + 66.60 100.3 67.30 + 66.70 99.96 67.11 + 66.80 99.61 66.91 + 66.90 99.26 66.72 + 67.00 98.91 66.52 + 67.10 97.17 66.33 + 67.20 95.43 66.13 + 67.30 93.70 65.93 + 67.40 91.96 65.74 + 67.50 90.22 65.54 + 67.60 88.48 65.35 + 67.70 86.74 65.15 + 67.80 85.00 64.96 + 67.90 83.26 64.76 + 68.00 81.52 64.57 + 68.10 78.61 64.48 + 68.20 75.70 64.39 + 68.30 72.78 64.30 + 68.40 69.87 64.22 + 68.50 66.96 64.13 + 68.60 64.04 64.04 + 68.70 61.13 63.96 + 68.80 58.22 63.87 + 68.90 55.30 63.78 + 69.00 52.39 63.70 + 69.10 51.39 63.61 + 69.20 50.39 63.52 + 69.30 49.39 63.43 + 69.40 48.39 63.35 + 69.50 47.39 63.26 + 69.60 47.43 63.17 + 69.70 47.48 63.09 + 69.80 47.52 63.00 + 69.90 47.57 62.91 + 70.00 47.61 62.83 + 70.10 48.53 62.63 + 70.20 49.46 62.43 + 70.30 50.38 62.24 + 70.40 51.30 62.04 + 70.50 52.68 61.85 + 70.60 54.06 61.65 + 70.70 55.43 61.46 + 70.80 56.81 61.26 + 70.90 58.19 61.07 + 71.00 59.57 60.87 + 71.10 60.94 60.67 + 71.20 62.32 60.48 + 71.30 63.70 60.28 + 71.40 65.07 60.09 + 71.50 66.45 59.89 + 71.60 67.83 59.70 + 71.70 69.20 59.50 + 71.80 70.58 59.30 + 71.90 71.96 59.11 + 72.00 71.96 58.91 + 72.10 71.96 58.74 + 72.20 71.96 58.57 + 72.30 71.96 58.39 + 72.40 71.22 58.22 + 72.50 70.49 58.04 + 72.60 69.76 57.87 + 72.70 69.02 57.70 + 72.80 68.29 57.52 + 72.90 67.55 57.35 + 73.00 66.82 57.17 + 73.10 66.09 57.00 + 73.20 64.43 56.83 + 73.30 62.77 56.65 + 73.40 61.11 56.48 + 73.50 59.46 56.30 + 73.60 57.80 56.13 + 73.70 56.14 55.96 + 73.80 54.48 55.78 + 73.90 53.65 55.61 + 74.00 52.83 55.43 + 74.10 52.17 55.32 + 74.20 51.52 55.20 + 74.30 50.87 55.08 + 74.40 50.22 54.96 + 74.50 49.57 54.84 + 74.60 48.91 54.72 + 74.70 48.26 54.60 + 74.80 47.61 54.48 + 74.90 46.96 54.36 + 75.00 46.30 54.24 + 75.10 45.65 54.12 + 75.20 45.33 54.00 + 75.30 45.00 53.88 + 75.40 44.67 53.76 + 75.50 44.35 53.64 + 75.60 44.02 53.52 + 75.70 43.70 53.40 + 75.80 43.37 53.28 + 75.90 43.21 53.16 + 76.00 43.04 53.04 + 76.10 43.02 52.97 + 76.20 43.00 52.89 + 76.30 42.98 52.82 + 76.40 42.96 52.74 + 76.50 42.93 52.66 + 76.60 42.91 52.59 + 76.70 42.89 52.51 + 76.80 42.87 52.43 + 76.90 42.85 52.36 + 77.00 42.83 52.28 + 77.10 42.96 52.21 + 77.20 43.09 52.13 + 77.30 43.22 52.05 + 77.40 43.35 51.98 + 77.50 43.48 51.90 + 77.60 43.61 51.83 + 77.70 43.74 51.75 + 77.80 43.87 51.67 + 77.90 44.00 51.60 + 78.00 44.13 51.52 + 78.10 44.21 51.50 + 78.20 44.29 51.48 + 78.30 44.37 51.46 + 78.40 44.45 51.43 + 78.50 44.53 51.41 + 78.60 44.60 51.39 + 78.70 44.68 51.37 + 78.80 44.76 51.35 + 78.90 44.84 51.33 + 79.00 44.92 51.30 + 79.10 45.00 51.28 + 79.20 44.97 51.26 + 79.30 44.95 51.24 + 79.40 44.92 51.22 + 79.50 44.89 51.20 + 79.60 44.86 51.17 + 79.70 44.84 51.15 + 79.80 44.81 51.13 + 79.90 44.80 51.11 + 80.00 44.78 51.09 + 80.10 44.63 51.01 + 80.20 44.48 50.93 + 80.30 44.33 50.86 + 80.40 44.17 50.78 + 80.50 44.02 50.71 + 80.60 43.87 50.63 + 80.70 43.72 50.55 + 80.80 43.57 50.48 + 80.90 43.41 50.40 + 81.00 43.26 50.33 + 81.10 43.11 50.25 + 81.20 42.96 50.17 + 81.30 42.80 50.10 + 81.40 42.65 50.02 + 81.50 42.50 49.95 + 81.60 42.35 49.87 + 81.70 42.20 49.79 + 81.80 42.04 49.72 + 81.90 41.89 49.64 + 82.00 41.74 49.57 + 82.10 41.78 49.53 + 82.20 41.83 49.50 + 82.30 41.87 49.47 + 82.40 41.91 49.43 + 82.50 41.96 49.40 + 82.60 42.00 49.37 + 82.70 42.04 49.34 + 82.80 42.09 49.30 + 82.90 42.13 49.27 + 83.00 42.17 49.24 + 83.10 42.50 49.21 + 83.20 42.83 49.17 + 83.30 43.15 49.14 + 83.40 43.48 49.11 + 83.50 43.80 49.08 + 83.60 44.13 49.04 + 83.70 44.46 49.01 + 83.80 44.78 48.98 + 83.90 45.11 48.95 + 84.00 45.43 48.91 + 84.10 45.91 49.01 + 84.20 46.39 49.10 + 84.30 46.87 49.19 + 84.40 47.35 49.29 + 84.50 47.83 49.38 + 84.60 48.30 49.47 + 84.70 48.78 49.57 + 84.80 49.26 49.66 + 84.90 49.74 49.75 + 85.00 50.22 49.84 + 85.10 50.29 49.94 + 85.20 50.36 50.03 + 85.30 50.43 50.12 + 85.40 50.51 50.22 + 85.50 50.58 50.31 + 85.60 50.65 50.40 + 85.70 50.72 50.50 + 85.80 50.80 50.59 + 85.90 50.87 50.68 + 86.00 50.48 50.78 + 86.10 50.09 50.87 + 86.20 49.70 51.29 + 86.30 49.30 51.71 + 86.40 48.91 52.14 + 86.50 48.52 52.56 + 86.60 48.13 52.98 + 86.70 47.74 53.41 + 86.80 47.35 53.83 + 86.90 47.15 54.25 + 87.00 46.96 54.67 + 87.10 46.96 55.10 + 87.20 46.96 55.52 + 87.30 46.96 55.94 + 87.40 46.96 56.36 + 87.50 47.52 56.79 + 87.60 48.09 57.21 + 87.70 48.65 57.63 + 87.80 49.22 58.06 + 87.90 49.50 58.26 + 88.00 49.78 58.48 + 88.10 52.45 58.89 + 88.20 55.12 59.31 + 88.30 57.80 59.72 + 88.40 60.47 60.14 + 88.50 63.14 60.55 + 88.60 65.81 60.97 + 88.70 68.48 61.38 + 88.80 70.54 61.80 + 88.90 72.61 62.21 + 89.00 74.67 62.63 + 89.10 76.74 63.04 + 89.20 78.22 62.74 + 89.30 79.70 62.45 + 89.40 81.17 62.15 + 89.50 82.65 61.85 + 89.60 83.39 61.55 + 89.70 84.13 61.25 + 89.80 83.96 60.95 + 89.90 83.78 60.75 + 90.00 83.61 60.65 + 90.10 83.43 60.02 + 90.20 83.26 59.39 + 90.30 81.89 58.76 + 90.40 80.53 58.13 + 90.50 79.16 57.50 + 90.60 77.80 56.87 + 90.70 76.43 56.24 + 90.80 75.06 55.61 + 90.90 74.38 54.98 + 91.00 73.70 54.35 + 91.10 72.48 53.85 + 91.20 71.26 53.35 + 91.30 70.04 52.85 + 91.40 68.83 52.35 + 91.50 67.61 51.85 + 91.60 66.39 51.35 + 91.70 65.17 50.85 + 91.80 63.96 50.35 + 91.90 62.74 49.85 + 92.00 61.52 49.35 + 92.10 61.57 49.13 + 92.20 61.62 48.91 + 92.30 61.67 48.70 + 92.40 61.71 48.48 + 92.50 61.76 48.26 + 92.60 61.81 48.04 + 92.70 61.86 47.83 + 92.80 61.91 47.61 + 92.90 61.96 47.39 + 93.00 61.94 47.17 + 93.10 61.92 46.96 + 93.20 61.90 46.74 + 93.30 61.88 46.52 + 93.40 61.87 46.30 + 93.50 61.85 46.09 + 93.60 61.83 45.87 + 93.70 61.81 45.65 + 93.80 61.79 45.43 + 93.90 61.78 45.22 + 94.00 61.76 45.00 + 94.10 61.74 44.82 + 94.20 61.57 44.63 + 94.30 61.41 44.45 + 94.40 61.24 44.26 + 94.50 61.07 44.08 + 94.60 60.91 43.89 + 94.70 60.74 43.71 + 94.80 60.58 43.52 + 94.90 60.41 43.34 + 95.00 60.24 43.15 + 95.10 60.08 42.97 + 95.20 59.91 42.78 + 95.30 59.74 42.60 + 95.40 59.58 42.41 + 95.50 59.41 42.23 + 95.60 59.25 42.04 + 95.70 59.08 41.86 + 95.80 58.91 41.67 + 95.90 58.46 41.49 + 96.00 58.01 41.30 + 96.10 57.56 41.25 + 96.20 57.11 41.20 + 96.30 56.66 41.14 + 96.40 56.20 41.09 + 96.50 55.75 41.03 + 96.60 55.30 40.98 + 96.70 54.85 40.92 + 96.80 54.40 40.87 + 96.90 53.95 40.82 + 97.00 53.49 40.76 + 97.10 53.27 40.71 + 97.20 53.04 40.65 + 97.30 52.27 40.60 + 97.40 51.49 40.54 + 97.50 50.71 40.49 + 97.60 49.94 40.43 + 97.70 49.16 40.38 + 97.80 48.39 40.33 + 97.90 48.00 40.27 + 98.00 47.61 40.22 + 98.10 46.24 40.17 + 98.20 44.87 40.13 + 98.30 43.50 40.09 + 98.40 42.13 40.04 + 98.50 40.76 40.00 + 98.60 39.39 39.96 + 98.70 38.02 39.91 + 98.80 36.65 39.87 + 98.90 35.28 39.83 + 99.00 33.91 39.78 + 99.10 33.53 39.74 + 99.20 33.14 39.70 + 99.30 32.75 39.65 + 99.40 32.37 39.61 + 99.50 31.98 39.57 + 99.60 31.59 39.52 + 99.70 31.21 39.48 + 99.80 30.82 39.43 + 99.90 30.43 39.39 + 100.0 30.51 39.35 + 100.1 30.58 39.32 + 100.2 30.65 39.29 + 100.3 30.72 39.26 + 100.4 30.80 39.23 + 100.5 30.87 39.21 + 100.6 30.94 39.18 + 100.7 31.01 39.15 + 100.8 31.09 39.12 + 100.9 31.38 39.09 + 101.0 31.68 39.06 + 101.1 31.98 39.03 + 101.2 32.27 39.01 + 101.3 32.57 38.98 + 101.4 32.87 38.95 + 101.5 33.16 38.92 + 101.6 33.46 38.89 + 101.7 33.75 38.86 + 101.8 34.05 38.83 + 101.9 34.20 38.81 + 102.0 34.35 38.78 + 102.1 34.62 38.75 + 102.2 34.90 38.72 + 102.3 35.17 38.69 + 102.4 35.45 38.66 + 102.5 35.72 38.63 + 102.6 36.00 38.61 + 102.7 36.27 38.58 + 102.8 36.54 38.55 + 102.9 36.82 38.52 + 103.0 37.09 38.49 + 103.1 37.37 38.46 + 103.2 37.64 38.43 + 103.3 37.92 38.41 + 103.4 38.19 38.38 + 103.5 38.47 38.35 + 103.6 38.74 38.32 + 103.7 39.02 38.29 + 103.8 39.29 38.26 + 103.9 39.57 38.23 + 104.0 39.61 38.21 + 104.1 39.65 38.18 + 104.2 39.70 38.15 + 104.3 39.74 38.12 + 104.4 39.78 38.09 + 104.5 39.83 38.06 + 104.6 39.87 38.03 + 104.7 39.91 38.01 + 104.8 39.96 37.98 + 104.9 40.00 37.95 + 105.0 39.71 37.92 + 105.1 39.41 37.89 + 105.2 39.12 37.86 + 105.3 38.83 37.83 + 105.4 38.53 37.81 + 105.5 38.24 37.78 + 105.6 37.95 37.75 + 105.7 37.65 37.72 + 105.8 37.36 37.69 + 105.9 37.07 37.66 + 106.0 36.77 37.64 + 106.1 36.48 37.61 + 106.2 36.18 37.58 + 106.3 35.89 37.55 + 106.4 35.60 37.52 + 106.5 35.30 37.49 + 106.6 35.01 37.46 + 106.7 34.72 37.44 + 106.8 34.42 37.41 + 106.9 34.13 37.38 + 107.0 34.15 37.35 + 107.1 34.17 37.32 + 107.2 34.20 37.29 + 107.3 34.22 37.26 + 107.4 34.24 37.24 + 107.5 34.26 37.21 + 107.6 34.28 37.18 + 107.7 34.30 37.15 + 107.8 34.33 37.12 + 107.9 34.34 37.09 + 108.0 34.35 37.06 + 108.1 34.61 37.04 + 108.2 34.87 37.01 + 108.3 35.13 36.98 + 108.4 35.39 36.95 + 108.5 35.65 36.92 + 108.6 35.91 36.89 + 108.7 36.17 36.86 + 108.8 36.43 36.84 + 108.9 36.70 36.81 + 109.0 36.96 36.78 + 109.1 36.93 36.75 + 109.2 36.91 36.72 + 109.3 36.89 36.69 + 109.4 36.87 36.66 + 109.5 36.85 36.64 + 109.6 36.83 36.61 + 109.7 36.80 36.58 + 109.8 36.78 36.55 + 109.9 36.76 36.52 + 110.0 36.74 36.52 Index: trunk/HiggsBounds-5/Expt_tables/ATLtables/336_Atlas_X-HH-bbtautau_13TeV_36.1fb-1.txt =================================================================== --- trunk/HiggsBounds-5/Expt_tables/ATLtables/336_Atlas_X-HH-bbtautau_13TeV_36.1fb-1.txt (revision 0) +++ trunk/HiggsBounds-5/Expt_tables/ATLtables/336_Atlas_X-HH-bbtautau_13TeV_36.1fb-1.txt (revision 587) @@ -0,0 +1,154 @@ +# ATLAS, arXiv:1808.00336, August 2018, Fig. 2(top) +# 336_Atlas_X-HH-bbtautau_13TeV_36.1fb-1.txt +# limit set on sigma(pp->X)xBR(X->HH)xBR(H->tautau)xBR(H->bb) x 2 (in pb) +# MX obs exp + + 260.0 0.1069 0.1870 + 265.0 0.1228 0.1938 + 270.0 0.1388 0.2007 + 275.0 0.1547 0.2075 + 280.0 0.1641 0.2003 + 285.0 0.1735 0.1932 + 290.0 0.1829 0.1860 + 295.0 0.1923 0.1789 + 300.0 0.2017 0.1717 + 305.0 0.1903 0.1600 + 310.0 0.1789 0.1483 + 315.0 0.1675 0.1366 + 320.0 0.1562 0.1249 + 325.0 0.1448 0.1132 + 330.0 0.1302 0.1093 + 335.0 0.1156 0.1054 + 340.0 0.1010 0.1014 + 345.0 0.8641E-01 0.9754E-01 + 350.0 0.7182E-01 0.9363E-01 + 355.0 0.6855E-01 0.8874E-01 + 360.0 0.6529E-01 0.8385E-01 + 365.0 0.6202E-01 0.7896E-01 + 370.0 0.5876E-01 0.7407E-01 + 375.0 0.5549E-01 0.6918E-01 + 380.0 0.5223E-01 0.6429E-01 + 385.0 0.4896E-01 0.5939E-01 + 390.0 0.4570E-01 0.5450E-01 + 395.0 0.4243E-01 0.4961E-01 + 400.0 0.3917E-01 0.4472E-01 + 405.0 0.3817E-01 0.4269E-01 + 410.0 0.3717E-01 0.4065E-01 + 415.0 0.3618E-01 0.3862E-01 + 420.0 0.3518E-01 0.3659E-01 + 425.0 0.3418E-01 0.3456E-01 + 430.0 0.3319E-01 0.3252E-01 + 435.0 0.3219E-01 0.3049E-01 + 440.0 0.3119E-01 0.2846E-01 + 445.0 0.3020E-01 0.2642E-01 + 450.0 0.2920E-01 0.2439E-01 + 455.0 0.2889E-01 0.2368E-01 + 460.0 0.2857E-01 0.2298E-01 + 465.0 0.2826E-01 0.2228E-01 + 470.0 0.2794E-01 0.2157E-01 + 475.0 0.2763E-01 0.2087E-01 + 480.0 0.2732E-01 0.2016E-01 + 485.0 0.2700E-01 0.1946E-01 + 490.0 0.2669E-01 0.1875E-01 + 495.0 0.2638E-01 0.1805E-01 + 500.0 0.2606E-01 0.1734E-01 + 505.0 0.2420E-01 0.1688E-01 + 510.0 0.2234E-01 0.1641E-01 + 515.0 0.2048E-01 0.1594E-01 + 520.0 0.1862E-01 0.1548E-01 + 525.0 0.1676E-01 0.1501E-01 + 530.0 0.1490E-01 0.1455E-01 + 535.0 0.1304E-01 0.1408E-01 + 540.0 0.1118E-01 0.1362E-01 + 545.0 0.9323E-02 0.1315E-01 + 550.0 0.7463E-02 0.1269E-01 + 555.0 0.7619E-02 0.1259E-01 + 560.0 0.7774E-02 0.1250E-01 + 565.0 0.7930E-02 0.1241E-01 + 570.0 0.8086E-02 0.1232E-01 + 575.0 0.8241E-02 0.1222E-01 + 580.0 0.8397E-02 0.1213E-01 + 585.0 0.8553E-02 0.1204E-01 + 590.0 0.8709E-02 0.1195E-01 + 595.0 0.8864E-02 0.1185E-01 + 600.0 0.9020E-02 0.1176E-01 + 605.0 0.9069E-02 0.1164E-01 + 610.0 0.9119E-02 0.1151E-01 + 615.0 0.9168E-02 0.1139E-01 + 620.0 0.9218E-02 0.1126E-01 + 625.0 0.9268E-02 0.1114E-01 + 630.0 0.9317E-02 0.1102E-01 + 635.0 0.9367E-02 0.1089E-01 + 640.0 0.9416E-02 0.1077E-01 + 645.0 0.9466E-02 0.1064E-01 + 650.0 0.9515E-02 0.1052E-01 + 655.0 0.9565E-02 0.1040E-01 + 660.0 0.9614E-02 0.1027E-01 + 665.0 0.9664E-02 0.1015E-01 + 670.0 0.9713E-02 0.1002E-01 + 675.0 0.9763E-02 0.9900E-02 + 680.0 0.9812E-02 0.9776E-02 + 685.0 0.9862E-02 0.9652E-02 + 690.0 0.9911E-02 0.9528E-02 + 695.0 0.9961E-02 0.9404E-02 + 700.0 0.1001E-01 0.9280E-02 + 705.0 0.9992E-02 0.9218E-02 + 710.0 0.9973E-02 0.9157E-02 + 715.0 0.9955E-02 0.9096E-02 + 720.0 0.9936E-02 0.9034E-02 + 725.0 0.9917E-02 0.8973E-02 + 730.0 0.9899E-02 0.8911E-02 + 735.0 0.9880E-02 0.8850E-02 + 740.0 0.9862E-02 0.8788E-02 + 745.0 0.9843E-02 0.8727E-02 + 750.0 0.9824E-02 0.8665E-02 + 755.0 0.9806E-02 0.8604E-02 + 760.0 0.9787E-02 0.8542E-02 + 765.0 0.9769E-02 0.8481E-02 + 770.0 0.9750E-02 0.8419E-02 + 775.0 0.9731E-02 0.8358E-02 + 780.0 0.9713E-02 0.8296E-02 + 785.0 0.9694E-02 0.8235E-02 + 790.0 0.9676E-02 0.8174E-02 + 795.0 0.9657E-02 0.8112E-02 + 800.0 0.9638E-02 0.8051E-02 + 805.0 0.9448E-02 0.8025E-02 + 810.0 0.9258E-02 0.7999E-02 + 815.0 0.9068E-02 0.7973E-02 + 820.0 0.8877E-02 0.7947E-02 + 825.0 0.8687E-02 0.7921E-02 + 830.0 0.8497E-02 0.7896E-02 + 835.0 0.8307E-02 0.7870E-02 + 840.0 0.8116E-02 0.7844E-02 + 845.0 0.7926E-02 0.7818E-02 + 850.0 0.7736E-02 0.7792E-02 + 855.0 0.7546E-02 0.7767E-02 + 860.0 0.7356E-02 0.7741E-02 + 865.0 0.7165E-02 0.7715E-02 + 870.0 0.6975E-02 0.7689E-02 + 875.0 0.6785E-02 0.7663E-02 + 880.0 0.6595E-02 0.7637E-02 + 885.0 0.6404E-02 0.7612E-02 + 890.0 0.6214E-02 0.7586E-02 + 895.0 0.6024E-02 0.7560E-02 + 900.0 0.5834E-02 0.7534E-02 + 905.0 0.6038E-02 0.7538E-02 + 910.0 0.6242E-02 0.7541E-02 + 915.0 0.6446E-02 0.7545E-02 + 920.0 0.6650E-02 0.7548E-02 + 925.0 0.6854E-02 0.7552E-02 + 930.0 0.7058E-02 0.7556E-02 + 935.0 0.7263E-02 0.7559E-02 + 940.0 0.7467E-02 0.7563E-02 + 945.0 0.7671E-02 0.7566E-02 + 950.0 0.7875E-02 0.7570E-02 + 955.0 0.8079E-02 0.7574E-02 + 960.0 0.8283E-02 0.7577E-02 + 965.0 0.8487E-02 0.7581E-02 + 970.0 0.8691E-02 0.7584E-02 + 975.0 0.8896E-02 0.7588E-02 + 980.0 0.9100E-02 0.7591E-02 + 985.0 0.9304E-02 0.7595E-02 + 990.0 0.9508E-02 0.7599E-02 + 995.0 0.9712E-02 0.7602E-02 + 1000. 0.9916E-02 0.7606E-02 Index: trunk/HiggsBounds-5/Expt_tables/ATLtables/8567_Atlas_X-HH-WWgaga_13TeV_36.1fb-1.txt =================================================================== --- trunk/HiggsBounds-5/Expt_tables/ATLtables/8567_Atlas_X-HH-WWgaga_13TeV_36.1fb-1.txt (revision 0) +++ trunk/HiggsBounds-5/Expt_tables/ATLtables/8567_Atlas_X-HH-WWgaga_13TeV_36.1fb-1.txt (revision 587) @@ -0,0 +1,246 @@ +# ATLAS, arXiv:1807.08567, July 2018, Fig. 4b +# 8567_Atlas_X-HH-WWgaga_13TeV_36.1fb-1.txt +# limit set on sigma(pp->X) x BR(X->HH) x BR(H->WW) x BR(H->gaga) x 2 [symmetryfactor] in pb +# MX obs exp + + 260.0 0.3944E-01 0.1726E-01 + 261.0 0.3928E-01 0.1720E-01 + 262.0 0.3912E-01 0.1713E-01 + 263.0 0.3896E-01 0.1707E-01 + 264.0 0.3879E-01 0.1700E-01 + 265.0 0.3863E-01 0.1694E-01 + 266.0 0.3847E-01 0.1687E-01 + 267.0 0.3831E-01 0.1681E-01 + 268.0 0.3814E-01 0.1674E-01 + 269.0 0.3798E-01 0.1667E-01 + 270.0 0.3782E-01 0.1661E-01 + 271.0 0.3766E-01 0.1654E-01 + 272.0 0.3750E-01 0.1648E-01 + 273.0 0.3733E-01 0.1641E-01 + 274.0 0.3717E-01 0.1635E-01 + 275.0 0.3701E-01 0.1628E-01 + 276.0 0.3685E-01 0.1622E-01 + 277.0 0.3668E-01 0.1615E-01 + 278.0 0.3652E-01 0.1609E-01 + 279.0 0.3636E-01 0.1602E-01 + 280.0 0.3620E-01 0.1596E-01 + 281.0 0.3604E-01 0.1589E-01 + 282.0 0.3587E-01 0.1583E-01 + 283.0 0.3571E-01 0.1576E-01 + 284.0 0.3555E-01 0.1570E-01 + 285.0 0.3539E-01 0.1563E-01 + 286.0 0.3522E-01 0.1556E-01 + 287.0 0.3506E-01 0.1550E-01 + 288.0 0.3490E-01 0.1543E-01 + 289.0 0.3474E-01 0.1537E-01 + 290.0 0.3458E-01 0.1530E-01 + 291.0 0.3441E-01 0.1524E-01 + 292.0 0.3425E-01 0.1517E-01 + 293.0 0.3409E-01 0.1511E-01 + 294.0 0.3393E-01 0.1504E-01 + 295.0 0.3376E-01 0.1498E-01 + 296.0 0.3360E-01 0.1491E-01 + 297.0 0.3344E-01 0.1485E-01 + 298.0 0.3328E-01 0.1478E-01 + 299.0 0.3312E-01 0.1472E-01 + 300.0 0.3295E-01 0.1465E-01 + 301.0 0.3279E-01 0.1459E-01 + 302.0 0.3263E-01 0.1452E-01 + 303.0 0.3247E-01 0.1446E-01 + 304.0 0.3230E-01 0.1439E-01 + 305.0 0.3214E-01 0.1432E-01 + 306.0 0.3198E-01 0.1426E-01 + 307.0 0.3182E-01 0.1419E-01 + 308.0 0.3166E-01 0.1413E-01 + 309.0 0.3149E-01 0.1406E-01 + 310.0 0.3133E-01 0.1400E-01 + 311.0 0.3117E-01 0.1393E-01 + 312.0 0.3101E-01 0.1387E-01 + 313.0 0.3084E-01 0.1380E-01 + 314.0 0.3068E-01 0.1374E-01 + 315.0 0.3052E-01 0.1367E-01 + 316.0 0.3036E-01 0.1361E-01 + 317.0 0.3020E-01 0.1354E-01 + 318.0 0.3003E-01 0.1348E-01 + 319.0 0.2987E-01 0.1341E-01 + 320.0 0.2971E-01 0.1335E-01 + 321.0 0.2955E-01 0.1328E-01 + 322.0 0.2938E-01 0.1321E-01 + 323.0 0.2922E-01 0.1315E-01 + 324.0 0.2906E-01 0.1308E-01 + 325.0 0.2890E-01 0.1302E-01 + 326.0 0.2874E-01 0.1295E-01 + 327.0 0.2857E-01 0.1289E-01 + 328.0 0.2841E-01 0.1282E-01 + 329.0 0.2825E-01 0.1276E-01 + 330.0 0.2809E-01 0.1269E-01 + 331.0 0.2792E-01 0.1263E-01 + 332.0 0.2776E-01 0.1256E-01 + 333.0 0.2760E-01 0.1250E-01 + 334.0 0.2744E-01 0.1243E-01 + 335.0 0.2728E-01 0.1237E-01 + 336.0 0.2711E-01 0.1230E-01 + 337.0 0.2695E-01 0.1224E-01 + 338.0 0.2679E-01 0.1217E-01 + 339.0 0.2663E-01 0.1211E-01 + 340.0 0.2646E-01 0.1204E-01 + 341.0 0.2630E-01 0.1197E-01 + 342.0 0.2614E-01 0.1191E-01 + 343.0 0.2598E-01 0.1184E-01 + 344.0 0.2582E-01 0.1178E-01 + 345.0 0.2565E-01 0.1171E-01 + 346.0 0.2549E-01 0.1165E-01 + 347.0 0.2533E-01 0.1158E-01 + 348.0 0.2517E-01 0.1152E-01 + 349.0 0.2500E-01 0.1145E-01 + 350.0 0.2484E-01 0.1139E-01 + 351.0 0.2474E-01 0.1134E-01 + 352.0 0.2465E-01 0.1130E-01 + 353.0 0.2455E-01 0.1126E-01 + 354.0 0.2445E-01 0.1122E-01 + 355.0 0.2435E-01 0.1117E-01 + 356.0 0.2426E-01 0.1113E-01 + 357.0 0.2416E-01 0.1109E-01 + 358.0 0.2406E-01 0.1105E-01 + 359.0 0.2396E-01 0.1100E-01 + 360.0 0.2387E-01 0.1096E-01 + 361.0 0.2377E-01 0.1092E-01 + 362.0 0.2367E-01 0.1088E-01 + 363.0 0.2357E-01 0.1083E-01 + 364.0 0.2348E-01 0.1079E-01 + 365.0 0.2338E-01 0.1075E-01 + 366.0 0.2328E-01 0.1071E-01 + 367.0 0.2318E-01 0.1066E-01 + 368.0 0.2309E-01 0.1062E-01 + 369.0 0.2299E-01 0.1058E-01 + 370.0 0.2289E-01 0.1054E-01 + 371.0 0.2279E-01 0.1049E-01 + 372.0 0.2270E-01 0.1045E-01 + 373.0 0.2260E-01 0.1041E-01 + 374.0 0.2250E-01 0.1037E-01 + 375.0 0.2240E-01 0.1032E-01 + 376.0 0.2231E-01 0.1028E-01 + 377.0 0.2221E-01 0.1024E-01 + 378.0 0.2211E-01 0.1020E-01 + 379.0 0.2201E-01 0.1015E-01 + 380.0 0.2191E-01 0.1011E-01 + 381.0 0.2182E-01 0.1007E-01 + 382.0 0.2172E-01 0.1003E-01 + 383.0 0.2162E-01 0.9983E-02 + 384.0 0.2152E-01 0.9940E-02 + 385.0 0.2143E-01 0.9898E-02 + 386.0 0.2133E-01 0.9855E-02 + 387.0 0.2123E-01 0.9813E-02 + 388.0 0.2113E-01 0.9770E-02 + 389.0 0.2104E-01 0.9727E-02 + 390.0 0.2094E-01 0.9685E-02 + 391.0 0.2084E-01 0.9642E-02 + 392.0 0.2074E-01 0.9600E-02 + 393.0 0.2065E-01 0.9557E-02 + 394.0 0.2055E-01 0.9515E-02 + 395.0 0.2045E-01 0.9472E-02 + 396.0 0.2035E-01 0.9430E-02 + 397.0 0.2026E-01 0.9387E-02 + 398.0 0.2016E-01 0.9344E-02 + 399.0 0.2006E-01 0.9302E-02 + 400.0 0.9142E-02 0.6316E-02 + 401.0 0.9111E-02 0.6296E-02 + 402.0 0.9080E-02 0.6275E-02 + 403.0 0.9049E-02 0.6255E-02 + 404.0 0.9018E-02 0.6235E-02 + 405.0 0.8986E-02 0.6214E-02 + 406.0 0.8955E-02 0.6194E-02 + 407.0 0.8924E-02 0.6174E-02 + 408.0 0.8893E-02 0.6154E-02 + 409.0 0.8862E-02 0.6133E-02 + 410.0 0.8831E-02 0.6113E-02 + 411.0 0.8800E-02 0.6093E-02 + 412.0 0.8769E-02 0.6073E-02 + 413.0 0.8738E-02 0.6052E-02 + 414.0 0.8706E-02 0.6032E-02 + 415.0 0.8675E-02 0.6012E-02 + 416.0 0.8644E-02 0.5991E-02 + 417.0 0.8613E-02 0.5971E-02 + 418.0 0.8582E-02 0.5951E-02 + 419.0 0.8551E-02 0.5931E-02 + 420.0 0.8520E-02 0.5910E-02 + 421.0 0.8489E-02 0.5890E-02 + 422.0 0.8458E-02 0.5870E-02 + 423.0 0.8426E-02 0.5850E-02 + 424.0 0.8395E-02 0.5829E-02 + 425.0 0.8364E-02 0.5809E-02 + 426.0 0.8333E-02 0.5789E-02 + 427.0 0.8302E-02 0.5768E-02 + 428.0 0.8271E-02 0.5748E-02 + 429.0 0.8240E-02 0.5728E-02 + 430.0 0.8209E-02 0.5708E-02 + 431.0 0.8177E-02 0.5687E-02 + 432.0 0.8146E-02 0.5667E-02 + 433.0 0.8115E-02 0.5647E-02 + 434.0 0.8084E-02 0.5627E-02 + 435.0 0.8053E-02 0.5606E-02 + 436.0 0.8022E-02 0.5586E-02 + 437.0 0.7991E-02 0.5566E-02 + 438.0 0.7960E-02 0.5545E-02 + 439.0 0.7929E-02 0.5525E-02 + 440.0 0.7897E-02 0.5505E-02 + 441.0 0.7866E-02 0.5485E-02 + 442.0 0.7835E-02 0.5464E-02 + 443.0 0.7804E-02 0.5444E-02 + 444.0 0.7773E-02 0.5424E-02 + 445.0 0.7742E-02 0.5403E-02 + 446.0 0.7711E-02 0.5383E-02 + 447.0 0.7680E-02 0.5363E-02 + 448.0 0.7649E-02 0.5343E-02 + 449.0 0.7617E-02 0.5322E-02 + 450.0 0.7586E-02 0.5302E-02 + 451.0 0.7555E-02 0.5282E-02 + 452.0 0.7524E-02 0.5262E-02 + 453.0 0.7493E-02 0.5241E-02 + 454.0 0.7462E-02 0.5221E-02 + 455.0 0.7431E-02 0.5201E-02 + 456.0 0.7400E-02 0.5180E-02 + 457.0 0.7368E-02 0.5160E-02 + 458.0 0.7337E-02 0.5140E-02 + 459.0 0.7306E-02 0.5120E-02 + 460.0 0.7275E-02 0.5099E-02 + 461.0 0.7244E-02 0.5079E-02 + 462.0 0.7213E-02 0.5059E-02 + 463.0 0.7182E-02 0.5039E-02 + 464.0 0.7151E-02 0.5018E-02 + 465.0 0.7120E-02 0.4998E-02 + 466.0 0.7088E-02 0.4978E-02 + 467.0 0.7057E-02 0.4957E-02 + 468.0 0.7026E-02 0.4937E-02 + 469.0 0.6995E-02 0.4917E-02 + 470.0 0.6964E-02 0.4897E-02 + 471.0 0.6933E-02 0.4876E-02 + 472.0 0.6902E-02 0.4856E-02 + 473.0 0.6871E-02 0.4836E-02 + 474.0 0.6840E-02 0.4816E-02 + 475.0 0.6808E-02 0.4795E-02 + 476.0 0.6777E-02 0.4775E-02 + 477.0 0.6746E-02 0.4755E-02 + 478.0 0.6715E-02 0.4734E-02 + 479.0 0.6684E-02 0.4714E-02 + 480.0 0.6653E-02 0.4694E-02 + 481.0 0.6622E-02 0.4674E-02 + 482.0 0.6591E-02 0.4653E-02 + 483.0 0.6559E-02 0.4633E-02 + 484.0 0.6528E-02 0.4613E-02 + 485.0 0.6497E-02 0.4592E-02 + 486.0 0.6466E-02 0.4572E-02 + 487.0 0.6435E-02 0.4552E-02 + 488.0 0.6404E-02 0.4532E-02 + 489.0 0.6373E-02 0.4511E-02 + 490.0 0.6342E-02 0.4491E-02 + 491.0 0.6311E-02 0.4471E-02 + 492.0 0.6279E-02 0.4451E-02 + 493.0 0.6248E-02 0.4430E-02 + 494.0 0.6217E-02 0.4410E-02 + 495.0 0.6186E-02 0.4390E-02 + 496.0 0.6155E-02 0.4369E-02 + 497.0 0.6124E-02 0.4349E-02 + 498.0 0.6093E-02 0.4329E-02 + 499.0 0.6062E-02 0.4309E-02 + 500.0 0.6031E-02 0.4288E-02 Index: trunk/HiggsBounds-5/Expt_tables/ATLtables/539_Atlas_H-aa-bbmumu_13TeV_36.1fb-1.txt =================================================================== --- trunk/HiggsBounds-5/Expt_tables/ATLtables/539_Atlas_H-aa-bbmumu_13TeV_36.1fb-1.txt (revision 0) +++ trunk/HiggsBounds-5/Expt_tables/ATLtables/539_Atlas_H-aa-bbmumu_13TeV_36.1fb-1.txt (revision 587) @@ -0,0 +1,86 @@ +# ATLAS, arXiv:1807.00539, July 2018, Fig. 6a +# 539_Atlas_H-aa-bbmumu_13TeV_36.1fb-1.txt +# Limit set on SM-normalized sigma(H) x BR(H-> aa -> bbmumu) +# Ma obs exp + + 20.00 0.3258E-03 0.2615E-03 + 20.50 0.3584E-03 0.2575E-03 + 21.00 0.3909E-03 0.2534E-03 + 21.50 0.3533E-03 0.2464E-03 + 22.00 0.3157E-03 0.2395E-03 + 22.50 0.2459E-03 0.2425E-03 + 23.00 0.1760E-03 0.2456E-03 + 23.50 0.1535E-03 0.2374E-03 + 24.00 0.1310E-03 0.2292E-03 + 24.50 0.1249E-03 0.2189E-03 + 25.00 0.1189E-03 0.2086E-03 + 25.50 0.1243E-03 0.2126E-03 + 26.00 0.1298E-03 0.2166E-03 + 26.50 0.1292E-03 0.2146E-03 + 27.00 0.1286E-03 0.2125E-03 + 27.50 0.2144E-03 0.2245E-03 + 28.00 0.3003E-03 0.2365E-03 + 28.50 0.3100E-03 0.2426E-03 + 29.00 0.3197E-03 0.2487E-03 + 29.50 0.2578E-03 0.2479E-03 + 30.00 0.1959E-03 0.2471E-03 + 30.50 0.2385E-03 0.2543E-03 + 31.00 0.2811E-03 0.2615E-03 + 31.50 0.2509E-03 0.2640E-03 + 32.00 0.2207E-03 0.2665E-03 + 32.50 0.2176E-03 0.2733E-03 + 33.00 0.2145E-03 0.2802E-03 + 33.50 0.2215E-03 0.2941E-03 + 34.00 0.2285E-03 0.3079E-03 + 34.50 0.2458E-03 0.3179E-03 + 35.00 0.2631E-03 0.3279E-03 + 35.50 0.3539E-03 0.3380E-03 + 36.00 0.4447E-03 0.3481E-03 + 36.50 0.5164E-03 0.3582E-03 + 37.00 0.5881E-03 0.3683E-03 + 37.50 0.6275E-03 0.3784E-03 + 38.00 0.6668E-03 0.3885E-03 + 38.50 0.5462E-03 0.3897E-03 + 39.00 0.4255E-03 0.3909E-03 + 39.50 0.4688E-03 0.4049E-03 + 40.00 0.5122E-03 0.4189E-03 + 40.50 0.6167E-03 0.4353E-03 + 41.00 0.7213E-03 0.4517E-03 + 41.50 0.7561E-03 0.4560E-03 + 42.00 0.6282E-03 0.4603E-03 + 42.50 0.4971E-03 0.4490E-03 + 43.00 0.3660E-03 0.4377E-03 + 43.50 0.3226E-03 0.4377E-03 + 44.00 0.2793E-03 0.4377E-03 + 44.50 0.2750E-03 0.4505E-03 + 45.00 0.3217E-03 0.4632E-03 + 45.50 0.4162E-03 0.4872E-03 + 46.00 0.5106E-03 0.5112E-03 + 46.50 0.5606E-03 0.5352E-03 + 47.00 0.6107E-03 0.5593E-03 + 47.50 0.6295E-03 0.5540E-03 + 48.00 0.6482E-03 0.5488E-03 + 48.50 0.6472E-03 0.5337E-03 + 49.00 0.6462E-03 0.5186E-03 + 49.50 0.7518E-03 0.5443E-03 + 50.00 0.8573E-03 0.5699E-03 + 50.50 0.8655E-03 0.5681E-03 + 51.00 0.7876E-03 0.5663E-03 + 51.50 0.6991E-03 0.5536E-03 + 52.00 0.6107E-03 0.5409E-03 + 52.50 0.5148E-03 0.5282E-03 + 53.00 0.4189E-03 0.5155E-03 + 53.50 0.3582E-03 0.5028E-03 + 54.00 0.2974E-03 0.4901E-03 + 54.50 0.2924E-03 0.4827E-03 + 55.00 0.2873E-03 0.4752E-03 + 55.50 0.3012E-03 0.4677E-03 + 56.00 0.3150E-03 0.4603E-03 + 56.50 0.3289E-03 0.4513E-03 + 57.00 0.3504E-03 0.4422E-03 + 57.50 0.3719E-03 0.4332E-03 + 58.00 0.3934E-03 0.4242E-03 + 58.50 0.3885E-03 0.4117E-03 + 59.00 0.3836E-03 0.3991E-03 + 59.50 0.3599E-03 0.3866E-03 + 60.00 0.3362E-03 0.3741E-03 Index: trunk/HiggsBounds-5/Expt_tables/CMStables/17013_CMS_H-gaga_lowmass_8TeV_20fb-1_and_13TeV_36fb-1.txt =================================================================== --- trunk/HiggsBounds-5/Expt_tables/CMStables/17013_CMS_H-gaga_lowmass_8TeV_20fb-1_and_13TeV_36fb-1.txt (revision 0) +++ trunk/HiggsBounds-5/Expt_tables/CMStables/17013_CMS_H-gaga_lowmass_8TeV_20fb-1_and_13TeV_36fb-1.txt (revision 587) @@ -0,0 +1,306 @@ +# CMS-PAS-HIG 17-013, Sept. 2017 +# 17013_CMS_H-gaga_lowmass_8TeV_20fb-1_and_13TeV_36fb-1 +# 8+13 TeV combination, Fig. 6 +# Mh observed expected (SM-normalized cross section) + + 80.00 0.6988 0.5522 + 80.10 0.6937 0.5507 + 80.20 0.6885 0.5492 + 80.30 0.6834 0.5476 + 80.40 0.6782 0.5461 + 80.50 0.6762 0.5445 + 80.60 0.6742 0.5430 + 80.70 0.6722 0.5415 + 80.80 0.6702 0.5399 + 80.90 0.6681 0.5384 + 81.00 0.6661 0.5368 + 81.10 0.6651 0.5353 + 81.20 0.6641 0.5337 + 81.30 0.6591 0.5322 + 81.40 0.6542 0.5307 + 81.50 0.6492 0.5291 + 81.60 0.6443 0.5276 + 81.70 0.6393 0.5260 + 81.80 0.6343 0.5245 + 81.90 0.6294 0.5229 + 82.00 0.6163 0.5214 + 82.10 0.6032 0.5197 + 82.20 0.5900 0.5181 + 82.30 0.5769 0.5164 + 82.40 0.5638 0.5147 + 82.50 0.5515 0.5130 + 82.60 0.5392 0.5114 + 82.70 0.5269 0.5097 + 82.80 0.5146 0.5080 + 82.90 0.5023 0.5064 + 83.00 0.4900 0.5047 + 83.10 0.4838 0.5030 + 83.20 0.4777 0.5013 + 83.30 0.4672 0.4997 + 83.40 0.4567 0.4980 + 83.50 0.4463 0.4963 + 83.60 0.4358 0.4947 + 83.70 0.4253 0.4930 + 83.80 0.4149 0.4913 + 83.90 0.4044 0.4896 + 84.00 0.3977 0.4880 + 84.10 0.3910 0.4863 + 84.20 0.3844 0.4846 + 84.30 0.3777 0.4830 + 84.40 0.3710 0.4813 + 84.50 0.3665 0.4796 + 84.60 0.3642 0.4779 + 84.70 0.3620 0.4763 + 84.80 0.3601 0.4746 + 84.90 0.3591 0.4729 + 85.00 0.3581 0.4713 + 85.10 0.3588 0.4702 + 85.20 0.3594 0.4692 + 85.30 0.3601 0.4682 + 85.40 0.3607 0.4671 + 85.50 0.3649 0.4661 + 85.60 0.3691 0.4651 + 85.70 0.3734 0.4641 + 85.80 0.3776 0.4630 + 85.90 0.3818 0.4620 + 86.00 0.3860 0.4610 + 86.10 0.3882 0.4607 + 86.20 0.3903 0.4603 + 86.30 0.3969 0.4600 + 86.40 0.4036 0.4597 + 86.50 0.4103 0.4594 + 86.60 0.4169 0.4590 + 86.70 0.4236 0.4587 + 86.80 0.4302 0.4584 + 86.90 0.4369 0.4610 + 87.00 0.4436 0.4635 + 87.10 0.4502 0.4661 + 87.20 0.4569 0.4687 + 87.30 0.4635 0.4707 + 87.40 0.4738 0.4713 + 87.50 0.4841 0.4758 + 87.60 0.5111 0.4804 + 87.70 0.5195 0.4850 + 87.80 0.5236 0.4896 + 87.90 0.5278 0.4942 + 88.00 0.5443 0.4988 + 88.10 0.5607 0.5034 + 88.20 0.5772 0.5170 + 88.30 0.5936 0.5307 + 88.40 0.6101 0.5443 + 88.50 0.6459 0.5579 + 88.60 0.6817 0.5679 + 88.70 0.7175 0.5715 + 88.80 0.7534 0.5887 + 88.90 0.7892 0.6058 + 89.00 0.8250 0.6230 + 89.10 0.8608 0.6401 + 89.20 0.8984 0.6572 + 89.30 0.9361 0.6744 + 89.40 0.9737 0.7007 + 89.50 1.011 0.7271 + 89.60 1.049 0.7534 + 89.70 1.087 0.7798 + 89.80 1.124 0.8062 + 89.90 1.137 0.8202 + 90.00 1.149 0.8325 + 90.10 1.135 0.8385 + 90.20 1.122 0.8445 + 90.30 1.109 0.8505 + 90.40 1.050 0.8454 + 90.50 0.9906 0.8424 + 90.60 0.9371 0.8402 + 90.70 0.8835 0.8171 + 90.80 0.8299 0.7939 + 90.90 0.7764 0.7702 + 91.00 0.7228 0.7466 + 91.10 0.6692 0.7229 + 91.20 0.6152 0.6992 + 91.30 0.5612 0.6755 + 91.40 0.5426 0.6518 + 91.50 0.5240 0.6368 + 91.60 0.4520 0.6281 + 91.70 0.4173 0.6062 + 91.80 0.3999 0.5844 + 91.90 0.3826 0.5625 + 92.00 0.3594 0.5407 + 92.10 0.3363 0.5188 + 92.20 0.3251 0.5078 + 92.30 0.3140 0.4968 + 92.40 0.3084 0.4858 + 92.50 0.3028 0.4747 + 92.60 0.3009 0.4637 + 92.70 0.2990 0.4527 + 92.80 0.3388 0.4417 + 92.90 0.3521 0.4368 + 93.00 0.3654 0.4319 + 93.10 0.3721 0.4270 + 93.20 0.3787 0.4221 + 93.30 0.4070 0.4173 + 93.40 0.4353 0.4124 + 93.50 0.4635 0.4075 + 93.60 0.4918 0.4026 + 93.70 0.5371 0.3977 + 93.80 0.5823 0.3928 + 93.90 0.6276 0.3909 + 94.00 0.6728 0.3890 + 94.10 0.6955 0.3871 + 94.20 0.7181 0.3851 + 94.30 0.7702 0.3832 + 94.40 0.7962 0.3813 + 94.50 0.8222 0.3793 + 94.60 0.8441 0.3774 + 94.70 0.8659 0.3755 + 94.80 0.8846 0.3745 + 94.90 0.8939 0.3736 + 95.00 0.9032 0.3726 + 95.10 0.9071 0.3717 + 95.20 0.9109 0.3707 + 95.30 0.9071 0.3698 + 95.40 0.9051 0.3688 + 95.50 0.9032 0.3679 + 95.60 0.8972 0.3670 + 95.70 0.8912 0.3660 + 95.80 0.8852 0.3651 + 95.90 0.8792 0.3641 + 96.00 0.8732 0.3632 + 96.10 0.8672 0.3622 + 96.20 0.8554 0.3613 + 96.30 0.8436 0.3604 + 96.40 0.8317 0.3604 + 96.50 0.8199 0.3594 + 96.60 0.8140 0.3587 + 96.70 0.8081 0.3580 + 96.80 0.8008 0.3573 + 96.90 0.7935 0.3566 + 97.00 0.7862 0.3559 + 97.10 0.7789 0.3552 + 97.20 0.7717 0.3545 + 97.30 0.7644 0.3538 + 97.40 0.7412 0.3531 + 97.50 0.7181 0.3524 + 97.60 0.6949 0.3518 + 97.70 0.6718 0.3511 + 97.80 0.6487 0.3504 + 97.90 0.6054 0.3497 + 98.00 0.5621 0.3490 + 98.10 0.5405 0.3483 + 98.20 0.5188 0.3476 + 98.30 0.4909 0.3469 + 98.40 0.4629 0.3462 + 98.50 0.4349 0.3455 + 98.60 0.4070 0.3448 + 98.70 0.3581 0.3441 + 98.80 0.3337 0.3434 + 98.90 0.3093 0.3427 + 99.00 0.2958 0.3418 + 99.10 0.2823 0.3410 + 99.20 0.2688 0.3401 + 99.30 0.2553 0.3392 + 99.40 0.2441 0.3384 + 99.50 0.2330 0.3375 + 99.60 0.2274 0.3366 + 99.70 0.2219 0.3357 + 99.80 0.2195 0.3349 + 99.90 0.2172 0.3340 + 100.0 0.2149 0.3331 + 100.1 0.2126 0.3323 + 100.2 0.2103 0.3314 + 100.3 0.2111 0.3305 + 100.4 0.2120 0.3297 + 100.5 0.2129 0.3288 + 100.6 0.2137 0.3279 + 100.7 0.2146 0.3270 + 100.8 0.2154 0.3262 + 100.9 0.2159 0.3253 + 101.0 0.2165 0.3244 + 101.1 0.2170 0.3236 + 101.2 0.2175 0.3227 + 101.3 0.2180 0.3218 + 101.4 0.2159 0.3210 + 101.5 0.2137 0.3201 + 101.6 0.2126 0.3192 + 101.7 0.2116 0.3183 + 101.8 0.2072 0.3175 + 101.9 0.2028 0.3166 + 102.0 0.1985 0.3157 + 102.1 0.1941 0.3149 + 102.2 0.1897 0.3140 + 102.3 0.1869 0.3131 + 102.4 0.1841 0.3122 + 102.5 0.1812 0.3113 + 102.6 0.1784 0.3104 + 102.7 0.1756 0.3095 + 102.8 0.1753 0.3086 + 102.9 0.1749 0.3077 + 103.0 0.1746 0.3068 + 103.1 0.1743 0.3059 + 103.2 0.1779 0.3050 + 103.3 0.1815 0.3041 + 103.4 0.1851 0.3032 + 103.5 0.1887 0.3023 + 103.6 0.1905 0.3014 + 103.7 0.1923 0.3005 + 103.8 0.2004 0.2996 + 103.9 0.2084 0.2987 + 104.0 0.2165 0.2978 + 104.1 0.2246 0.2968 + 104.2 0.2327 0.2959 + 104.3 0.2408 0.2950 + 104.4 0.2448 0.2941 + 104.5 0.2489 0.2932 + 104.6 0.2567 0.2923 + 104.7 0.2646 0.2914 + 104.8 0.2725 0.2905 + 104.9 0.2804 0.2896 + 105.0 0.2883 0.2896 + 105.1 0.2962 0.2887 + 105.2 0.3041 0.2880 + 105.3 0.3080 0.2873 + 105.4 0.3118 0.2867 + 105.5 0.3157 0.2860 + 105.6 0.3196 0.2853 + 105.7 0.3234 0.2846 + 105.8 0.3247 0.2839 + 105.9 0.3253 0.2832 + 106.0 0.3260 0.2826 + 106.1 0.3237 0.2819 + 106.2 0.3215 0.2812 + 106.3 0.3192 0.2805 + 106.4 0.3170 0.2798 + 106.5 0.3131 0.2791 + 106.6 0.3093 0.2784 + 106.7 0.3054 0.2778 + 106.8 0.3016 0.2771 + 106.9 0.2977 0.2764 + 107.0 0.2938 0.2757 + 107.1 0.2919 0.2750 + 107.2 0.2900 0.2743 + 107.3 0.2843 0.2737 + 107.4 0.2786 0.2730 + 107.5 0.2729 0.2723 + 107.6 0.2672 0.2716 + 107.7 0.2615 0.2709 + 107.8 0.2558 0.2702 + 107.9 0.2501 0.2696 + 108.0 0.2446 0.2689 + 108.1 0.2391 0.2682 + 108.2 0.2336 0.2675 + 108.3 0.2281 0.2668 + 108.4 0.2226 0.2661 + 108.5 0.2171 0.2655 + 108.6 0.2116 0.2648 + 108.7 0.2045 0.2641 + 108.8 0.2010 0.2634 + 108.9 0.1974 0.2627 + 109.0 0.1968 0.2620 + 109.1 0.1961 0.2614 + 109.2 0.1955 0.2607 + 109.3 0.1949 0.2600 + 109.4 0.1969 0.2593 + 109.5 0.1990 0.2586 + 109.6 0.2010 0.2579 + 109.7 0.2031 0.2572 + 109.8 0.2101 0.2572 + 109.9 0.2167 0.2579 + 110.0 0.2207 0.2585 Index: trunk/HiggsBounds-5/S95tables_type1.F90 =================================================================== --- trunk/HiggsBounds-5/S95tables_type1.F90 (revision 586) +++ trunk/HiggsBounds-5/S95tables_type1.F90 (revision 587) @@ -1,5424 +1,5510 @@ ! This file is part of HiggsBounds ! -KW !****************************************************************** module S95tables_type1 !****************************************************************** implicit none !table type 1----------------------------- type table1 integer :: id,nx,particle_x !see usefulbits.f90 for key to particle codes n.b. they're NOT pdg character(LEN=45) :: label character(LEN=100) :: desc character(LEN=3) :: expt double precision :: lumi, energy double precision :: xmax,xmin,sep,deltax integer :: SMlike integer :: llh double precision, allocatable :: dat(:,:) !in dat(a,b), a=row, b=1,2 for obs,pred end type !------------------------------------------ integer,parameter :: file_id_1=10 !same as file_id_common in usefulbits.f90 contains !************************************************************ subroutine initializetables_type1_blank(tablet1) !*********************************************************** ! still leaves dat unallocated integer:: i type(table1) :: tablet1(:) do i=lbound(tablet1,dim=1),ubound(tablet1,dim=1) tablet1(i)%id = -1 tablet1(i)%nx = -1 tablet1(i)%particle_x = -1 tablet1(i)%label = '' tablet1(i)%desc = '' tablet1(i)%expt = '' tablet1(i)%lumi = -1.0D0 tablet1(i)%energy = -1.0D0 tablet1(i)%xmax = -1.0D0 tablet1(i)%xmin = -1.0D0 tablet1(i)%sep = -1.0D0 tablet1(i)%deltax = -1.0D0 tablet1(i)%SMlike = 0 tablet1(i)%llh = 0 enddo end subroutine initializetables_type1_blank !************************************************************ subroutine copy_type1(tablet1_orig,tablet1_copy) !*********************************************************** ! note tablet1_1,tablet1_2 are not arrays ! still leaves dat uncopied type(table1) :: tablet1_orig type(table1) :: tablet1_copy tablet1_copy%id = tablet1_orig%id tablet1_copy%nx = tablet1_orig%nx tablet1_copy%particle_x = tablet1_orig%particle_x tablet1_copy%label = tablet1_orig%label tablet1_copy%expt = tablet1_orig%expt tablet1_copy%xmax = tablet1_orig%xmax tablet1_copy%xmin = tablet1_orig%xmin tablet1_copy%sep = tablet1_orig%sep tablet1_copy%deltax = tablet1_orig%deltax end subroutine copy_type1 !*********************************************************** function t1elementnumberfromid(t1,id) !--------------------------------------input type(table1), intent(in) :: t1(:) integer, intent(in) :: id !-----------------------------------function integer :: t1elementnumberfromid !-----------------------------------internal integer :: n,x !------------------------------------------- n=0 do x=lbound(t1,dim=1),ubound(t1,dim=1) if(t1(x)%id.eq.id)then n=n+1 t1elementnumberfromid=x endif enddo if(n.ne.1)stop 'problem in function t3elementnumberfromid 1' end function t1elementnumberfromid !************************************************************ subroutine initializetables1(S95_t1) !*********************************************************** ! fills S95_t1 !*********************************************************** use store_pathname use usefulbits, only: Hneut,Hplus,file_id_common2 implicit none !--------------------------------------input type(table1) :: S95_t1(:) !-----------------------------------internal logical :: newtables integer :: x,xbeg,xend character(len=100),allocatable :: filename(:) character(LEN=pathname_length+150) :: fullfilename integer :: col integer :: ios !------------------------------------------- xbeg=lbound(S95_t1,dim=1) xend=ubound(S95_t1,dim=1) allocate(filename(xbeg:xend)) x=xbeg-1 !instead, could read in the values of xmin,xmax,sep from the !files, but it's kinda nice having them all here to refer to newtables=.True. ! i.e. use the recommended LEP single Higgs tables if(newtables)then x=x+1 S95_t1(x)%id=142 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0602042, table 14b (LEP)' ! table 14b S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=12.0D0 S95_t1(x)%xmax=120.0D0 S95_t1(x)%sep=0.5D0 filename(x)='lep210_hbb' x=x+1 S95_t1(x)%id=143 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0602042, table 14c (LEP)' ! table 14c S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=4.0D0 S95_t1(x)%xmax=120.0D0 S95_t1(x)%sep=0.5D0 filename(x)='lep210_htt_interpol' else write(*,*)'WARNING: using old LEP tables' x=x+1 S95_t1(x)%id=142 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='LEP table 14b' ! table 14b S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=1.0D0 S95_t1(x)%xmax=140.0D0 S95_t1(x)%sep=0.1D0 filename(x)='old-s95_h2z_bbz' x=x+1 S95_t1(x)%id=143 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='LEP table 14c' ! table 14c S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=1.0D0 S95_t1(x)%xmax=140.0D0 S95_t1(x)%sep=0.1D0 filename(x)='old-s95_h2z_ttz' endif x=x+1 S95_t1(x)%id=300 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0206022 (OPAL)' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=1.0D0 S95_t1(x)%xmax=100.0D0 S95_t1(x)%sep=1.0D0 filename(x)='lep_decaymodeindep' x=x+1 S95_t1(x)%id=400 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0107032v1 (LEP)' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=118.0D0 S95_t1(x)%sep=1.0D0 filename(x)='LEP_h-invisible' x=x+1 S95_t1(x)%id=500 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='LHWG Note 2002-02' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=20.0D0 S95_t1(x)%xmax=116.0D0 S95_t1(x)%sep=2.0D0 filename(x)='LEP_h-gammagamma' x=x+1 S95_t1(x)%id=600 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='LHWG (unpublished)'!uses hep-ex/0510022,hep-ex/0205055,hep-ex/0312042,hep-ex/0408097 S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=20.0D0 S95_t1(x)%xmax=128.6D0 S95_t1(x)%sep=0.1D0 filename(x)='LEP_h-2jets' x=x+1 S95_t1(x)%id=601 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0107034 (LHWG)'!uses hep-ex/0510022,hep-ex/0205055,hep-ex/0312042,hep-ex/0408097 S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=60.0D0 S95_t1(x)%xmax=114.5D0 S95_t1(x)%sep=0.1D0 filename(x)='LEP_h-2jets_0107034' x=x+1 S95_t1(x)%id=711 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0410017 (DELPHI)' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=12.0D0 S95_t1(x)%xmax=50.0D0 S95_t1(x)%sep=1.0D0 filename(x)='Delphi_yuk_h_bbbb' x=x+1 S95_t1(x)%id=713 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0410017 (DELPHI)' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=12.0D0 S95_t1(x)%xmax=50.0D0 S95_t1(x)%sep=1.0D0 filename(x)='Delphi_yuk_a_bbbb' x=x+1 S95_t1(x)%id=721 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0410017 (DELPHI)' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=4.0D0 S95_t1(x)%xmax=50.0D0 S95_t1(x)%sep=1.0D0 filename(x)='Delphi_yuk_h_bbtautau' x=x+1 S95_t1(x)%id=741 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0111010 (OPAL)' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=4.0D0 S95_t1(x)%xmax=12.0D0 S95_t1(x)%sep=1.0D0 filename(x)='OPAL_yuk_h_bbtautau' x=x+1 S95_t1(x)%id=723 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0410017 (DELPHI)' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=4.0D0 S95_t1(x)%xmax=50.0D0 S95_t1(x)%sep=1.0D0 filename(x)='Delphi_yuk_a_bbtautau' x=x+1 S95_t1(x)%id=743 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0111010 (OPAL)' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=4.0D0 S95_t1(x)%xmax=12.0D0 S95_t1(x)%sep=1.0D0 filename(x)='OPAL_yuk_a_bbtautau' x=x+1 S95_t1(x)%id=731 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0410017 (DELPHI)' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=4.0D0 S95_t1(x)%xmax=27.0D0 S95_t1(x)%sep=1.0D0 filename(x)='Delphi_yuk_h_tautautautau' x=x+1 S95_t1(x)%id=733 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0410017 (DELPHI)' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=4.0D0 S95_t1(x)%xmax=26.0D0 S95_t1(x)%sep=1.0D0 filename(x)='Delphi_yuk_a_tautautautau' x=x+1 S95_t1(x)%id=402 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0401022 (Delphi)' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=40.0D0 S95_t1(x)%xmax=114.0D0 S95_t1(x)%sep=2.0D0 filename(x)='Delphi_h-invisible' x=x+1 S95_t1(x)%id=403 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0501033 (L3)' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=50.0D0 S95_t1(x)%xmax=110.0D0 S95_t1(x)%sep=5.0D0 filename(x)='L3_h-invisible' x=x+1 S95_t1(x)%id=401 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='LEP' S95_t1(x)%label='[hep-ex] arXiv:0707.0373 (OPAL)' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=5.0D0 S95_t1(x)%xmax=115.0D0 S95_t1(x)%sep=5.0D0 filename(x)='OPAL_h-invisible' !x=x+1 !S95_t1(x)%id=803 !S95_t1(x)%particle_x=Hplus !S95_t1(x)%expt='LEP' !S95_t1(x)%label='[hep-ex] arxiv:0812.0267 (OPAL)' !S95_t1(x)%xmin=50.0D0 !S95_t1(x)%xmax=93.0D0 !S95_t1(x)%sep=1.0D0 !filename(x)='OPAL_HpHm_taunutaunu' !x=x+1 !S95_t1(x)%id=802 !S95_t1(x)%particle_x=Hplus !S95_t1(x)%expt='LEP' !S95_t1(x)%label='[hep-ex] arxiv:0812.0267 (OPAL)' !S95_t1(x)%xmin=50.0D0 !S95_t1(x)%xmax=93.0D0 !S95_t1(x)%sep=1.0D0 !filename(x)='OPAL_HpHm_qqtaunu' !x=x+1 !S95_t1(x)%id=801 !S95_t1(x)%particle_x=Hplus !S95_t1(x)%expt='LEP' !S95_t1(x)%label='[hep-ex] arxiv:0812.0267 (OPAL)' !S95_t1(x)%xmin=50.0D0 !S95_t1(x)%xmax=93.0D0 !S95_t1(x)%sep=1.0D0 !filename(x)='OPAL_HpHm_qqqq' x=x+1 S95_t1(x)%id=821 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0107031 (LHWG)' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=60.0D0 S95_t1(x)%xmax=90.0D0 S95_t1(x)%sep=1.0D0 filename(x)='LEP_HpHm_qqqq' x=x+1 S95_t1(x)%id=811 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0404012 (Delphi)' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=52.0D0 S95_t1(x)%xmax=94.0D0 S95_t1(x)%sep=2.0D0 filename(x)='Delphi_HpHm_qqqq' x=x+1 S95_t1(x)%id=813 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='LEP' S95_t1(x)%label='hep-ex/0404012 (Delphi)' S95_t1(x)%energy=0.208D0 S95_t1(x)%xmin=52.0D0 S95_t1(x)%xmax=94.0D0 S95_t1(x)%sep=2.0D0 filename(x)='Delphi_HpHm_taunutaunu' !----------------------- Z H -> l l b b ------------------------- ! x=x+1 ! S95_t1(x)%id=10235 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CDF' ! S95_t1(x)%label='CDF Note 10235' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=5.7D0 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! filename(x)='CDF_ZH_llbb_5.7fb_10235' ! ! x=x+1 ! S95_t1(x)%id=3047 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CDF' ! S95_t1(x)%label='[hep-ex] arXiv:1009.3047 (CDF)' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=4.1D0 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! filename(x)='CDF_ZH_llbb_4.1fb_3047' x=x+1 S95_t1(x)%id=10799 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='CDF Note 10799' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=9.45D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=5.0D0 filename(x)='CDF_ZH_llbb_9.45fb_10799' ! x=x+1 ! S95_t1(x)%id=6166 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 6166' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=8.6D0 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! filename(x)='D0_ZH_llbb_8.6fb_6166' x=x+1 S95_t1(x)%id=6296 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 6296' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=9.7D0 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=5.0D0 filename(x)='D0_ZH_llbb_9.7fb_6296' !x=x+1 !S95_t1(x)%id=6089 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 6089' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='D0_ZH_llbb_6.2fb_6089' x=x+1 S95_t1(x)%id=3564 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='[hep-ex] arXiv:1008.3564 (D0)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=4.2D0 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=5.0D0 filename(x)='D0_ZH_llbb_4.2fb_3564' !x=x+1 !S95_t1(x)%id=10212 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 10212' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='CDF_VH_Metbb_5.7fb_10212' ! x=x+1 ! S95_t1(x)%id=6087 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 6087' ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='D0_VH_bb_6.4fb_6087' ! x=x+1 ! S95_t1(x)%id=2012015 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2012-015' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=4.7D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=130.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2012015_Atlas_VH_bb_ll_lnu_nunu_4.7fb-1' !----------------------- V H -> b b Etmiss ------------------------- ! x=x+1 ! S95_t1(x)%id=10583 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CDF' ! S95_t1(x)%label='CDF Note 10583' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=7.8D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='CDF_VH_Metbb_7.8fb_10583' ! x=x+1 ! S95_t1(x)%id=6223 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 6223' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=8.4D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='D0_VH_bb_8.4fb_6223' ! x=x+1 ! S95_t1(x)%id=3935 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CDF' ! S95_t1(x)%label='[hep-ex] arXiv:0911.3935v4 (CDF)' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=2.1D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='CDF_VH_Metbb_2.1fb_3935_interpol' ! ! x=x+1 ! S95_t1(x)%id=5285 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='[hep-ex] arXiv:0912.5285 (D0)' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=5.2D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='D0_VH_bb_5.2fb_5285' !x=x+1 !S95_t1(x)%id=6092 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 6092'!this is what the note says, but the website says 6082 !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='D0_WH_lnubb_5.3fb_6092' ! x=x+1 ! S95_t1(x)%id=10596 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CDF' ! S95_t1(x)%label='CDF Note 10596' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=7.5D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='CDF_VH_lnubb_7.5fb_10596' ! x=x+1 ! S95_t1(x)%id=2011103 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2011-103' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=1.04D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=130.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2011103_Atlas_VH_Vbb_1.04fb-1' x=x+1 S95_t1(x)%id=10798 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='CDF Note 10798' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=9.45D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='CDF_VH_Metbb_9.45fb_10798' x=x+1 S95_t1(x)%id=6299 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 6299' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=9.5D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_VH_bb_9.5fb_6299' x=x+1 S95_t1(x)%id=2012161 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2012-161' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=17.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=130.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2012161_Atlas_VH-Vbb_17.7fb-1' ! x=x+1 ! S95_t1(x)%id=11031 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-031' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=4.7D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=135.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11031_CMS_VH-bb_BDT_4.7fb-1' ! x=x+1 ! S95_t1(x)%id=12044 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-12-044' ! S95_t1(x)%energy=8.0D0 ! S95_t1(x)%lumi=17.1D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=135.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='12044_CMS_VH_Vbb_17.1fb-1' ! x=x+1 S95_t1(x)%id=13012 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-13-012' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=24.D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=135.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='13012_CMS_VH_bb_24fb-1' !----------------------- VBF(H), H -> b b ------------------------- x=x+1 S95_t1(x)%id=13011 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-13-011' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=115.0D0 S95_t1(x)%xmax=135.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='13011_CMS_VBF_bb_19fb-1' !----------------------- W H -> b b ------------------------- ! x=x+1 ! S95_t1(x)%id=6220 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 6220' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=8.5D0 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! filename(x)='D0_WH_lnubb_8.5fb_6220' x=x+1 S95_t1(x)%id=6309 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 6309' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=9.6D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_WH_lnubb_9.7_6309' ! x=x+1 ! S95_t1(x)%id=10239 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CDF' ! S95_t1(x)%label='CDF Note 10239' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=5.7D0 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! filename(x)='CDF_WH_lnubb_5.7fb_10239' x=x+1 S95_t1(x)%id=10796 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='CDF Note 10796' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=9.45D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=5.0D0 filename(x)='CDF_WH_lnubb_9.45fb_10796' x=x+1 S95_t1(x)%id=0874 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='[hep-ex] arXiv:1012.0874 (D0)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=5.3D0 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=5.0D0 filename(x)='D0_WH_lnubb_5.3fb_0874' x=x+1 S95_t1(x)%id=5613 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='[hep-ex] arXiv:0906.5613 (CDF)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=2.7D0 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=5.0D0 filename(x)='CDF_WH_lnubb_2.7fb_5613' !----------------------- V H, H -> invisible ------------------------- ! x=x+1 ! S95_t1(x)%id=2013011 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2013-011' ! S95_t1(x)%energy=8.0D0 ! S95_t1(x)%lumi=17.7D0 ! S95_t1(x)%xmin=115.0D0 ! S95_t1(x)%xmax=300.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2013011_Atlas_H-inv_17.7fb-1' x=x+1 S95_t1(x)%id=3244 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1402.3244 (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=24.8D0 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=400.0D0 S95_t1(x)%sep=0.1D0 S95_t1(x)%deltax=0.0D0 filename(x)='3244_Atlas_H-inv_24.8fb-1' ! x=x+1 ! S95_t1(x)%id=13018 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-13-018' ! S95_t1(x)%energy=8.0D0 ! S95_t1(x)%lumi=24.7D0 ! S95_t1(x)%xmin=105.0D0 ! S95_t1(x)%xmax=145.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='13018_CMS_ZH-inv_24.7fb-1' x=x+1 S95_t1(x)%id=13442 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='[hep-ex] arXiv:1404.1344 (CMS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=24.60 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=105.0D0 S95_t1(x)%xmax=145.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='1344_CMS_ZH-invisible_24.6fb-1' !----------------------- VBF, H -> invisible ------------------------- ! x=x+1 ! S95_t1(x)%id=13013 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-13-013' ! S95_t1(x)%energy=8.0D0 ! S95_t1(x)%lumi=19.6D0 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=400.0D0 ! S95_t1(x)%sep=10.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='13013_CMS_VBF-inv_19.6fb-1' x=x+1 S95_t1(x)%id=13441 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='[hep-ex] arXiv:1404.1344 (CMS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.5D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=400.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='1344_CMS_VBF-invisible_19.5fb-1' x=x+1 S95_t1(x)%id=13443 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='[hep-ex] arXiv:1404.1344 (CMS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%SMlike=1 S95_t1(x)%lumi=24.60 S95_t1(x)%xmin=115.0D0 S95_t1(x)%xmax=145.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='1344_CMS_ZH_VBF-invisible_24.6fb-1' + x=x+1 + S95_t1(x)%id=6682 + S95_t1(x)%particle_x=Hneut + S95_t1(x)%expt='ATL' + S95_t1(x)%label='[hep-ex] arXiv:1809.06682 (ATLAS)' + S95_t1(x)%energy=13.0D0 + S95_t1(x)%SMlike=0 + S95_t1(x)%lumi=36.1D0 + S95_t1(x)%xmin=75.0D0 + S95_t1(x)%xmax=3000.0D0 + S95_t1(x)%sep=5.0D0 + S95_t1(x)%deltax=5.0D0 + filename(x)='6682_Atlas_VBF_h-invisible_13TeV_36.1fb-1' + !----------------------- H -> W W ------------------------- x=x+1 S95_t1(x)%id=5757 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 5757' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=3.0D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=115.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_ppH_WW_ll_3.0fb_5757' x=x+1 S95_t1(x)%id=3930 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='[hep-ex] arXiv:0809.3930 (CDF)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=3.0D0 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=10.0D0 filename(x)='CDF_ggH_WW_3.0fb_3930' ! x=x+1 ! S95_t1(x)%id=3216 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='TCB' ! S95_t1(x)%label='[hep-ex] arXiv:1005.3216 (TEVNPHWG)' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=5.4D0 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=300.0D0 ! S95_t1(x)%sep=5.0D0 ! filename(x)='CDF_D0_combined_gg-H-WW_4.8-5.4fb_3216_bayesian_interpol' !x=x+1 !S95_t1(x)%id=10102 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 10102' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='CDF_H-WW_5.3fb_10102' ! x=x+1 ! S95_t1(x)%id=6221 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 6219' !this note has two results in it, both can not have the id 6219 ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=8.1D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=115.0D0 ! S95_t1(x)%xmax=300.0D0 ! S95_t1(x)%sep=5.0D0 ! filename(x)='D0_H-WW_8.1fb_6221_interpol' x=x+1 S95_t1(x)%id=6276 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 6276' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=9.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_H-VV_9.7fb_6276' x=x+1 S95_t1(x)%id=6301 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 6301' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=9.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=115.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=5.0D0 filename(x)='D0_VH_VWW_9.7fb_6301' x=x+1 S95_t1(x)%id=10600 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='CDF Note 10599' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=8.2D0 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=300.0D0 S95_t1(x)%sep=5.0D0 filename(x)='CDF_ggH-WW_8.2fb_10600_interpol' x=x+1 S95_t1(x)%id=10599 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='CDF Note 10599' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=8.2D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='CDF_H-WW_8.2fb_10599' x=x+1 S95_t1(x)%id=4468 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='[hep-ex] arXiv:1001.4468 (CDF)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=4.8D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='CDF_H-WW_4.8fb_4468_interpol' ! x=x+1 ! S95_t1(x)%id=5871 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 5871' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=4.2D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=115.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='D0_H-WW_llnunu_4.2fb_5871' !x=x+1 !S95_t1(x)%id=6082 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 6082' !S95_t1(x)%xmin=115.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='D0_H-VV_6.7fb_6082' ! x=x+1 ! S95_t1(x)%id=6219 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 6219' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=8.1D0 ! S95_t1(x)%xmin=115.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='D0_H-VV_8.1fb_6219' ! x=x+1 ! S95_t1(x)%id=6179 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 6179' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=7.3D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=115.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='D0_H-WW-mutau_7.3fb_6179' x=x+1 S95_t1(x)%id=6302 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 6302' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=9.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=115.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_H-WW_9.7fb_6302' x=x+1 S95_t1(x)%id=6183 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 6183' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=8.2D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=130.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_SM_combined_6183' x=x+1 S95_t1(x)%id=4481 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='[hep-ex] arXiv:1001.4481 (D0)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=5.4D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=115.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_H-WW_5.4fb_4481' ! x=x+1 ! S95_t1(x)%id=4162 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='TCB' ! S95_t1(x)%label='[hep-ex] arXiv:1001.4162 (TEVNPHWG)' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=5.4D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=130.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='CDF_D0_SM_combined_H-WW_4.8-5.4fb_4162' x=x+1 S95_t1(x)%id=3331 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='TCB' S95_t1(x)%label='[hep-ex] arXiv:1108.3331 (TEVNPHWG)'!CDF note 10608, D0 Note 6230 S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=8.2D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=300.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='CDF_D0_combined_gg-H-WW_8.2fb_3331_bayesian_interpol' ! x=x+1 ! S95_t1(x)%id=2011134 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2011-134' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=1.7D0 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=300.0D0 ! S95_t1(x)%sep=1.0D0 ! filename(x)='2011134_Atlas_H-WW-lnulnu_1.7fb-1_interpol' x=x+1 S95_t1(x)%id=2012012 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2012-012' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=4.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2012012_Atlas_H-WW-lnulnu_4.7fb-1' ! x=x+1 ! S95_t1(x)%id=2012158 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2012-158' ! S95_t1(x)%energy=8.0D0 ! S95_t1(x)%lumi=13.0D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=115.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2012158_Atlas_H-WW-enumunu_13fb-1' x=x+1 S95_t1(x)%id=2013030 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2013-030' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=25.0D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2013030_Atlas_H-WW-lnulnu_25fb-1' ! x=x+1 ! S95_t1(x)%id=5429 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='[hep-ex] arXiv: 1102.5429(CMS)' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=0.036D0 ! S95_t1(x)%xmin=130.0D0 ! S95_t1(x)%xmax=400.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='5429_CMS_H-WW_36pb-1_rat_interpol' x=x+1 S95_t1(x)%id=2577 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arxiv:1112.2577' S95_t1(x)%desc='pp->h + X->W W* + X ->l l nu nu' S95_t1(x)%energy=7.D0 S95_t1(x)%lumi=2.05D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=300.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2577_Atlas_H-WW-lnulnu_2.05fb-1' ! x=x+1 ! S95_t1(x)%id=1489 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='[hep-ex] arxiv:1202.1489 (CMS)' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=4.6D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=5D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11024_CMS_H-WW-lnulnu_4.6fb-1_interpol' ! x=x+1 ! S95_t1(x)%id=12042 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-12-042' ! S95_t1(x)%energy=8.0D0 ! S95_t1(x)%lumi=16.0D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=1D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='12042_CMS_H-WW-lnulnu_16.0fb-1' x=x+1 S95_t1(x)%id=13003 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-13-003' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=25.0D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=5D0 S95_t1(x)%deltax=0.0D0 filename(x)='13003_CMS_H-WW-lnulnu_25fb-1' x=x+1 S95_t1(x)%id=13027 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-13-027' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=24.3D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=170.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='13027_CMS_H-WW-lnujj_24.3fb-1' x=x+1 S95_t1(x)%id=13022 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-13-022' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=25.4D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=5D0 S95_t1(x)%deltax=0.0D0 filename(x)='13022_CMS_VBF-WW_25.4fb-1' x=x+1 S95_t1(x)%id=2016062 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATLAS' S95_t1(x)%label='ATLAS-CONF-2016-062' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=13.2D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=500.0D0 S95_t1(x)%xmax=3000.0D0 S95_t1(x)%sep=50.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='2016062_Atlas_gg-H-WW-lnuqq_13.2fb-1' !--------------- H -> VV -> l nu l nu ---------------- x=x+1 S95_t1(x)%id=3357 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1109.3357 (ATLAS)' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=1.04D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=200.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=20.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='3357_Atlas_H-ZZ-llnunu_1.04fb-1' ! x=x+1 ! S95_t1(x)%id=2011148 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2011-148' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=2.05D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=200.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=20.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2011148_Atlas_H-ZZ-lnulnu_2.05fb-1' x=x+1 S95_t1(x)%id=2012016 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2012-016' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=4.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=200.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2012016_Atlas_H-ZZ-llnunu_4.7fb-1' x=x+1 S95_t1(x)%id=3478 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='[hep-ex] arxiv:1202.3478 (CMS)' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=4.6D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=250.0D0 S95_t1(x)%xmax=590.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='11026_CMS_H-ZZ-llnunu_4.6fb-1' !----------------------- H -> W W ----------------------------- ! x=x+1 ! S95_t1(x)%id=2011052 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2011-052' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=0.035D0 ! S95_t1(x)%xmin=220.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=20.0D0 ! filename(x)='2011052_Atlas_H-WW_35pb-1' ! x=x+1 ! S95_t1(x)%id=3615 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='[hep-ex] arXiv:1109.3615 (ATLAS)' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=0.035D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=240.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=20.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='3615_Atlas_H-WW-lnuqq_1.04fb-1' ! ! x=x+1 ! S95_t1(x)%id=2012018 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2012-018' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=4.7D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=300.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=10.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2012018_Atlas_H-WW-lnuqq_4.7fb-1' x=x+1 S95_t1(x)%id=12046 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-12-046' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=17D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=170.0D0 S95_t1(x)%xmax=580.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='12046_CMS_H-WW-lnuqq_17fb-1' x=x+1 S95_t1(x)%id=20160741 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2016-074' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=13.2D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=300.0D0 S95_t1(x)%xmax=3000.0D0 S95_t1(x)%sep=50.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='2016074_Atlas_gg-H-WW-lnulnu_13.2fb-1' x=x+1 S95_t1(x)%id=20160742 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2016-074' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=13.2D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=300.0D0 S95_t1(x)%xmax=3000.0D0 S95_t1(x)%sep=50.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='2016074_Atlas_vbf-H-WW-lnulnu_13.2fb-1' !------------------------- H -> Z Z -------------------------- x=x+1 S95_t1(x)%id=5064 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1108.5064 (ATLAS)' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=1.04D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=200.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='5064_Atlas_H-ZZ-llqq_1.04fb-1' x=x+1 S95_t1(x)%id=2012017 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2012-017' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=4.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=200.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2012017_Atlas_H-ZZ-llqq_4.7fb-1' x=x+1 S95_t1(x)%id=14161 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='[hep-ex] arXiv:1202.1416 (CMS)' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=4.6D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=130.0D0 S95_t1(x)%xmax=164.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='110271_CMS_H-ZZ-llqq_4.6fb-1' x=x+1 S95_t1(x)%id=14162 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='[hep-ex] arXiv:1202.1416 (CMS)' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=4.6D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=200.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='110272_CMS_H-ZZ-llqq_4.6fb-1' x=x+1 S95_t1(x)%id=1415 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1202.1415 (ATLAS)' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=4.8D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='1415_Atlas_H-ZZ-4l_4.8fb-1' x=x+1 S95_t1(x)%id=2012092 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2012-092' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=10.6D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2012092_Atlas_H-ZZ-4l_10.6fb-1' x=x+1 S95_t1(x)%id=20130131 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2013-013' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=25.0D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=180.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2013013-1_Atlas_H-ZZ-4l_incl_25fb-1' x=x+1 S95_t1(x)%id=20130132 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2013-013' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=21.0D0 S95_t1(x)%xmin=200.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=5.0D0 filename(x)='2013013-2_Atlas_H-ZZ-4l_ggF_21fb-1' x=x+1 S95_t1(x)%id=20130133 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2013-013' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=21.0D0 S95_t1(x)%xmin=200.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=5.0D0 filename(x)='2013013-3_Atlas_H-ZZ-4l_VBFVH_21fb-1' x=x+1 S95_t1(x)%id=20160792 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2016-079' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=14.8D0 S95_t1(x)%xmin=200.0D0 S95_t1(x)%xmax=400.0D0 S95_t1(x)%sep=1.0D0 filename(x)='20160792_gg-H-ZZ-4l_14.8fb-1_lowmass' x=x+1 S95_t1(x)%id=20160793 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2016-079' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=14.8D0 S95_t1(x)%xmin=200.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=1.0D0 filename(x)='20160793_VBF-H-ZZ-4l_14.8fb-1' x=x+1 S95_t1(x)%id=1997 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='[hep-ex] arxiv:1202.1997 (CMS)' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=4.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='11025_CMS_H-ZZ-4l_4.7fb-1' ! x=x+1 ! S95_t1(x)%id=12041 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-12-041' ! S95_t1(x)%energy=8.0D0 ! S95_t1(x)%lumi=17.3D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='12041_CMS_H-ZZ-4l_17.3fb-1' x=x+1 S95_t1(x)%id=130021 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-13-002' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=25.0D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='13002-1_CMS_H-ZZ-4l_lowm_25fb-1' x=x+1 S95_t1(x)%id=130022 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-13-002' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=25.0D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=150.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='13002-2_CMS_H-ZZ-4l_highm_25fb-1' x=x+1 S95_t1(x)%id=009361 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='[hep-ex] arXiv:1504.00936 (CMS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=24.8D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=145.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='009361_CMS_H-VV_5.1fb-1_19.7fb-1' x=x+1 S95_t1(x)%id=063861 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='arXiv:1712.06386 (ATLAS)' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=36.1D0 S95_t1(x)%xmin=200.0D0 S95_t1(x)%xmax=400.0D0 S95_t1(x)%sep=1.0D0 filename(x)='063861_ATLAS_gg-H-ZZ-4l+2l2nu_NWA_36.1fb-1' x=x+1 S95_t1(x)%id=20160821 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2016-082' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=13.2D0 S95_t1(x)%xmin=500.0D0 S95_t1(x)%xmax=3000.0D0 S95_t1(x)%sep=1.0D0 filename(x)='20160821_Atlas_gg-H-ZZ-llnunu_13.2fb-1' x=x+1 S95_t1(x)%id=20160822 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2016-082' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=13.2D0 S95_t1(x)%xmin=300.0D0 S95_t1(x)%xmax=3000.0D0 S95_t1(x)%sep=1.0D0 filename(x)='20160822_Atlas_gg-H-ZZ-llqq_13.2fb-1' x=x+1 S95_t1(x)%id=20160823 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2016-082' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=13.2D0 S95_t1(x)%xmin=300.0D0 S95_t1(x)%xmax=3000.0D0 S95_t1(x)%sep=1.0D0 filename(x)='20160823_Atlas_qq-Hqq-ZZ-llqq_13.2fb-1' x=x+1 S95_t1(x)%id=16034 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-16-034' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=12.9D0 S95_t1(x)%xmin=550.0D0 S95_t1(x)%xmax=2000.0D0 S95_t1(x)%sep=10.0D0 filename(x)='16034_CMS_H-ZZ-llqq_12.9fb-1' !------------------------- SM combined ----------------------- ! x=x+1 ! S95_t1(x)%id=8961 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='TCB' ! S95_t1(x)%label='[hep-ex] arXiv:0712.2383v1(TEVNPHWG)' !CDF Note 8961, D0 Note 5536 ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=1.9D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='CDF_D0_SM_combined_1.0-1.9fb_8961-5536_interpol' x=x+1 S95_t1(x)%id=10439 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='CDF Note 10439' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=6.0D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='CDF_H-tautau_6.0fb_10439' !x=x+1 !S95_t1(x)%id=10133 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 10133' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='CDF_H-tautau_2.3fb_10133' ! x=x+1 ! S95_t1(x)%id=4800 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='[hep-ex] arXiv:0903.4800 (D0)' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=1.0D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=105.0D0 ! S95_t1(x)%xmax=145.0D0 ! S95_t1(x)%sep=10.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='D0_SM_tautau_1.0fb_4800' ! x=x+1 S95_t1(x)%id=5845 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 5845' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=4.9D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=105.0D0 S95_t1(x)%xmax=145.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_tautauqq_4.9fb_5845' ! x=x+1 ! S95_t1(x)%id=9290 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='TCB' ! S95_t1(x)%label='[hep-ex] arXiv:0804.3423(TEVNPHWG)' !CDF Note 9290, D0 Note 5645 ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=2.4D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='CDF_D0_SM_combined_1.0-2.4fb_9290-5645_interpol' ! x=x+1 ! S95_t1(x)%id=9465 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='TCB' ! S95_t1(x)%label='[hep-ex] arXiv:0808.0534(TEVNPHWG)' !CDF Note 9465, D0 Note 5754 ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=3.0D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=155.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! !filename(x)='CDF_D0_SM_combined_3.0fb_9465-5754_CLs' ! filename(x)='CDF_D0_SM_combined_3.0fb_9465-5754_bayesian' ! x=x+1 ! S95_t1(x)%id=0598 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='[hep-ex] arXiv:0712.0598v1 (D0)' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=0.44D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='D0_SM_combined_0598_interpol' x=x+1 S95_t1(x)%id=9999 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='CDF Note 9999' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=4.8D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='CDF_SM_combined_2.0-4.8fb_9999_interpol' ! x=x+1 ! S95_t1(x)%id=6008 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 6008' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=5.4D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='D0_SM_combined_6008' x=x+1 S95_t1(x)%id=6305 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 6305' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=7.3D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=105.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_H-tautau_7.3fb_6305' ! x=x+1 ! S95_t1(x)%id=9998 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='TCB' ! S95_t1(x)%label='[hep-ex] arXiv:0911.3930 (TEVNPHWG)'!CDF Note 9998, D0 Note 5983 ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=5.4D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='CDF_D0_SM_combined_2.1-5.4fb_9998-5983_bayesian' ! x=x+1 ! S95_t1(x)%id=6096 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='TCB' ! S95_t1(x)%label='[hep-ex] arXiv:1007.4587 (TEVNPHWG)' !CDF Note 10241, D0 Note 6096 ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=6.7D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='CDF_D0_SM_combined_2.1-6.7fb_10241-6096_bayesian' x=x+1 S95_t1(x)%id=10010 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='CDF Note 10010' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=4D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='CDF_hadr_4fb_10010' x=x+1 S95_t1(x)%id=6171 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 6171' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=4.3D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=105.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_H-tautaujj-4.3fb_6171' ! x=x+1 ! S95_t1(x)%id=6229 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 6229' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=8.6D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='D0_SM_combined_6229' x=x+1 S95_t1(x)%id=6304 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 6304' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=9.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_SM_combined_6304' x=x+1 S95_t1(x)%id=10500 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='CDF Note 10500' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=6.2D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='CDF_VH_tautau_6.2fb_10500' x=x+1 S95_t1(x)%id=10573 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='CDF Note 10573' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=8.2D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=120.0D0 S95_t1(x)%xmax=300.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='CDF_H-WW_8.2fb_10573' x=x+1 S95_t1(x)%id=6286 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 6286' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=7.0D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_tautaumu_7.0fb_6286' ! x=x+1 ! S95_t1(x)%id=3233 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='TCB' ! S95_t1(x)%label='[hep-ex] arXiv:1103.3233v2 (TEVNPHWG)' !CDF Note 10432, D0 Note 6183 ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=8.2D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=130.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! !filename(x)='CDF_D0_SM_combined_4.3-8.2fb_3233_CLs' ! filename(x)='CDF_D0_SM_combined_4.3-8.2fb_3233_bayesian' ! ! x=x+1 ! S95_t1(x)%id=10606 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='TCB' ! S95_t1(x)%label='[hep-ex] arXiv:1107.5518 (TEVNPHWG)' !CDF Note 10606, D0 Note 6226 ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=8.6D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='CDF_D0_SM_combined_8.6fb_10606' x=x+1 S95_t1(x)%id=10884 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='TCB' S95_t1(x)%label='[hep-ex] arXiv:1207.0449 (TEVNPHWG)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=10.D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='10884_CDF_D0_SM_combined_10fb-1' ! x=x+1 ! S95_t1(x)%id=10607 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='TCB' ! S95_t1(x)%label='[hep-ex] arXiv:1107.5518 (TEVNPHWG)' !CDF Note 10606, D0 Note 6226 ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=8.6D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='CDF_D0_combined_h-bb_8.6fb_10607' x=x+1 S95_t1(x)%id=6436 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='TCB' S95_t1(x)%label='[hep-ex] arXiv:1207.6436 (TEVNPHWG)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=9.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='1207.6436_CDF_D0_combined_h-bb_9.7fb-1' ! x=x+1 ! S95_t1(x)%id=2011112 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2011-112' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=1.21D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2011112_Atlas_SMcombined_1.04-1.21fb-1_interpol' ! ! x=x+1 ! S95_t1(x)%id=2011135 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2011-135' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=2.3D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2011135_Atlas_SMcombined_1-2.3fb-1_interpol' ! ! x=x+1 ! S95_t1(x)%id=2011163 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2011-163' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=4.9D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=0.5D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2011163_Atlas_SMcombined_4.9fb-1' ! x=x+1 S95_t1(x)%id=1408 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='(hep-ex) arxiv:1202.1408 (ATLAS)' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=4.9D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='1408_Atlas_SMcombined_4.9fb-1' x=x+1 S95_t1(x)%id=2012019 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2012-019' S95_t1(x)%desc='(p p)->h+...' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=4.9D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2012019_Atlas_SMcombined_4.9fb-1' x=x+1 S95_t1(x)%id=7214 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='(hep-ex) arXiv:1207.7214 (ATLAS)' S95_t1(x)%desc='(p p)->h+...' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=10.5D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=0.1D0 S95_t1(x)%deltax=0.0D0 filename(x)='7214_Atlas_SMcombined_10.5fb-1' x=x+1 S95_t1(x)%id=2011157 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2011-157, CMS-PAS-HIG-11-023' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=2.3D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2011157_Atlas_CMS_SMcombined_2.7fb-1' ! x=x+1 ! S95_t1(x)%id=11011 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-011' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=1.1D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=10.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11011_CMS_SMcomb_1.1fb-1_interpol' x=x+1 S95_t1(x)%id=1488 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='[hep-ex] arxiv:1202.1488 (CMS)' S95_t1(x)%energy=7.D0 S95_t1(x)%lumi=4.8D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='1488_CMS_SMcombined_4.8fb-1' ! x=x+1 ! S95_t1(x)%id=12008 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-12-008' ! S95_t1(x)%desc='(p p)->h+...' ! S95_t1(x)%energy=7.D0 ! S95_t1(x)%lumi=4.8D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='12008_CMS_SMcombined_4.8fb-1' x=x+1 S95_t1(x)%id=12045 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-12-045' S95_t1(x)%desc='(p p)->h+...' S95_t1(x)%energy=8.D0 S95_t1(x)%lumi=17.3D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='12045_CMS_SMcombined_17.3fb-1' !----------------- b H -> 3 b jets ------------------- ! x=x+1 ! S95_t1(x)%id=10105 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CDF' ! S95_t1(x)%label='CDF Note 10105' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=2.2D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=210.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='CDF_bbH_bb_2.2fb_10105' ! x=x+1 ! S95_t1(x)%id=5726 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 5726' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=2.6D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=220.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='D0_bbH_bb_2.6fb_5726_sq_interpol' x=x+1 S95_t1(x)%id=1931 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='[hep-ex] arXiv:1011.1931 (D0)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=5.2D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=300.0D0 S95_t1(x)%sep=10.0D0 filename(x)='D0_bbH_bb_5.2fb_1931' x=x+1 S95_t1(x)%id=4782 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='arXiv:1106.4782 (CDF)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=2.6D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=350.0D0 S95_t1(x)%sep=10.0D0 filename(x)='CDF_bbH_bb_2.6fb_4782' ! x=x+1 ! S95_t1(x)%id=12033 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-12-033' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=4.8D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=350.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='12033_CMS_bbH-bbbb_4.8fb-1' x=x+1 S95_t1(x)%id=1508329 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='arXiv:1506.08329 (CMS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.7D0 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=900.0D0 S95_t1(x)%sep=10.0D0 filename(x)='1508329_CMS_Hb-bbb_19.7fb-1' x=x+1 S95_t1(x)%id=2015080 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='CERN-THESIS-2015-080 (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.5D0 S95_t1(x)%xmin=450.0D0 S95_t1(x)%xmax=800.0D0 S95_t1(x)%sep=50.0D0 filename(x)='2015080_Atlas_hb-bbb_19.5fb-1' !-------------------- H -> tau tau ------------------------- x=x+1 S95_t1(x)%id=4555 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='[hep-ex] arXiv:1106.4555 (D0)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=5.4D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=300.0D0 S95_t1(x)%sep=10.0D0 filename(x)='D0_H-tautau_5.4fb_4555_interpol' ! x=x+1 ! S95_t1(x)%id=2491 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='[hep-ex] arXiv:0805.2491 (D0)' ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=300.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='D0_ppH_tautau_1fb_2491_interpol' x=x+1 S95_t1(x)%id=1014 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='[hep-ex] arXiv:0906.1014 (CDF)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=1.8D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=250.0D0 S95_t1(x)%sep=10.0D0 filename(x)='CDF_H-tautau_1.8fb_1014_interpol' ! x=x+1 ! S95_t1(x)%id=5740 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 5740' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=2.2D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=300.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='D0_H-tautau_2.2fb_5740_interpol' x=x+1 S95_t1(x)%id=3363 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='TCB' S95_t1(x)%label='[hep-ex] arXiv:1003.3363 (TEVNPHWG)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=2.2D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=10.0D0 filename(x)='CDF_D0_combinedH-tautau_2.2fb_3363_CLs' ! x=x+1 ! S95_t1(x)%id=2011133 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2011-133' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=1.06D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=140.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2011133_Atlas_H-tautau-ll4nu_1.06fb-1' ! x=x+1 ! S95_t1(x)%id=2012014 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2012-014' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=4.7D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2012014_Atlas_H-tautau_4.7fb-1' x=x+1 S95_t1(x)%id=2012160 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2012-160' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=17.6D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2012160_Atlas_H-tautau_17.6fb-1' ! x=x+1 ! S95_t1(x)%id=5003 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='[hep-ex] arXiv:1107.5003 (ATLAS)'!CERN-PH-EP-2011-104 ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=0.036D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=300.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='5003_Atlas_ggh_h-tautau_36pb-1' ! x=x+1 ! S95_t1(x)%id=2011132 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2011-132' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=1.06D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='2011132_Atlas_conserv_h-tautau_1.06fb-1_interpol' ! x=x+1 ! S95_t1(x)%id=2012094 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2012-094' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=4.7D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=500.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='2012094_Atlas_H-tautau_4.7fb-1' ! Analysis is disabled when using CMS tau tau likelihood x=x+1 S95_t1(x)%id=2014049 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2014-049, arXiv:1409.6064' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=20.3D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%llh=1 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=20.0D0 filename(x)='2014049_Atlas_bbh_h-tautau_20.3fb-1' ! Analysis is disabled when using CMS tau tau likelihood x=x+1 S95_t1(x)%id=20140492 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2014-049, arXiv:1409.6064' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=20.3D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%llh=1 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=20.0D0 filename(x)='20140492_Atlas_ggh_h-tautau_20.3fb-1' ! Analysis is disabled when using CMS tau tau likelihood ! x=x+1 ! S95_t1(x)%id=20160851 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2016-085' ! S95_t1(x)%energy=13.0D0 ! S95_t1(x)%lumi=13.3D0 ! S95_t1(x)%xmin=200.0D0 ! S95_t1(x)%xmax=1200.0D0 ! S95_t1(x)%llh=1 ! S95_t1(x)%sep=20.0D0 ! S95_t1(x)%deltax=20.0D0 ! filename(x)='20160851_Atlas_ggh_h_tautau_13.3fb-1' ! Analysis is disabled when using CMS tau tau likelihood ! x=x+1 ! S95_t1(x)%id=20160852 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2016-085' ! S95_t1(x)%energy=13.0D0 ! S95_t1(x)%lumi=13.3D0 ! S95_t1(x)%xmin=200.0D0 ! S95_t1(x)%xmax=1200.0D0 ! S95_t1(x)%llh=1 ! S95_t1(x)%sep=20.0D0 ! S95_t1(x)%deltax=20.0D0 ! filename(x)='20160852_Atlas_bbh_h_tautau_13.3fb-1' ! Analysis is disabled when using CMS tau tau likelihood ! x=x+1 ! S95_t1(x)%id=160371 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-16-037' ! S95_t1(x)%energy=13.0D0 ! S95_t1(x)%lumi=12.9D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=3000.0D0 ! S95_t1(x)%llh=1 ! S95_t1(x)%sep=10.0D0 ! S95_t1(x)%deltax=20.0D0 ! filename(x)='160371_CMS_ggh_h_tautau_12.9fb-1' ! Analysis is disabled when using CMS tau tau likelihood ! x=x+1 ! S95_t1(x)%id=160372 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-16-037' ! S95_t1(x)%energy=13.0D0 ! S95_t1(x)%lumi=12.9D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=3000.0D0 ! S95_t1(x)%llh=1 ! S95_t1(x)%sep=10.0D0 ! S95_t1(x)%deltax=20.0D0 ! filename(x)='160372_CMS_bbh_h_tautau_12.9fb-1' ! Analysis is disabled when using CMS tau tau likelihood ! x=x+1 ! S95_t1(x)%id=20170501 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2017-050' ! S95_t1(x)%energy=13.0D0 ! S95_t1(x)%lumi=36.1D0 ! S95_t1(x)%xmin=200.0D0 ! S95_t1(x)%xmax=2250.0D0 ! S95_t1(x)%llh=1 ! S95_t1(x)%sep=10.0D0 ! S95_t1(x)%deltax=20.0D0 ! filename(x)='20170501_Atlas_gg-H-tautau_36.1fb-1' ! x=x+1 ! S95_t1(x)%id=20170502 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2017-050' ! S95_t1(x)%energy=13.0D0 ! S95_t1(x)%lumi=36.1D0 ! S95_t1(x)%xmin=200.0D0 ! S95_t1(x)%xmax=2250.0D0 ! S95_t1(x)%llh=1 ! S95_t1(x)%sep=10.0D0 ! S95_t1(x)%deltax=20.0D0 ! filename(x)='20170502_Atlas_bb-H-tautau_36.1fb-1' ! x=x+1 ! S95_t1(x)%id=110291 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-029' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=4.6D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=145.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11029_CMS_H-tautau_4.6fb-1_SM' x=x+1 S95_t1(x)%id=12043 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-12-043' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=17.D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=145.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='12043_CMS_H_tautau_17fb-1' ! x=x+1 ! S95_t1(x)%id=10002 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='[hep-ex] arXiv: 1104:1619(CMS)'!CMS-PAS-HIG-10-002 ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=0.036D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=500.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='10002_CMS_H-tautau_36pb-1_interpol' ! x=x+1 ! S95_t1(x)%id=110292 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='[hep-ex] arXiv: 1202.4083 (CMS)' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=4.6D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=500.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='11029_CMS_H-tautau_4.6fb-1_MSSM_interpol' ! ! x=x+1 ! S95_t1(x)%id=12050 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-12-050' ! S95_t1(x)%energy=8.0D0 ! S95_t1(x)%lumi=17.D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=800.0D0 ! S95_t1(x)%sep=1.0D0 ! filename(x)='12050_CMS_H-tautau_17fb-1' ! Still in testing phase! ! x=x+1 ! S95_t1(x)%id=13021 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-13-021' ! S95_t1(x)%energy=8.0D0 ! S95_t1(x)%lumi=25.6D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=1000.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='13021_CMS_H-tautau_25.6fb-1_MSSM_ggH' !-------------------- Higgs to Higgs decays ------------------------- ! ! Requires hi -> hj Z branching ratio in input! ! x=x+1 S95_t1(x)%id=14011 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-14-011, arXiv:1504.04710 (CMS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.7D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=225.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=0.1D0 S95_t1(x)%deltax=10.0D0 filename(x)='14011_CMS_A-Zh-llbb_19.7fb-1' ! x=x+1 S95_t1(x)%id=04670 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1509.04670 (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=20.3D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=260.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=0.1D0 S95_t1(x)%deltax=10.0D0 filename(x)='04670_Atlas_H-hh-combined_20.3fb-1' x=x+1 S95_t1(x)%id=046701 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1509.04670 (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=20.3D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=260.0D0 S95_t1(x)%xmax=500.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='04670_Atlas_H-hh-gagaWW_20.3fb-1' x=x+1 + S95_t1(x)%id=8567 + S95_t1(x)%particle_x=Hneut + S95_t1(x)%expt='ATL' + S95_t1(x)%label='[hep-ex] arXiv:1807.08567 (ATLAS)' + S95_t1(x)%energy=13.0D0 + S95_t1(x)%lumi=36.1D0 + S95_t1(x)%SMlike=0 + S95_t1(x)%xmin=260.0D0 + S95_t1(x)%xmax=500.0D0 + S95_t1(x)%sep=1.0D0 + S95_t1(x)%deltax=10.0D0 + filename(x)='8567_Atlas_X-HH-WWgaga_13TeV_36.1fb-1' + + x=x+1 S95_t1(x)%id=4873 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1807.04873 (ATLAS)' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=36.1D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=260.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='4873_Atlas_X-HH-gagabb_13TeV_36.1fb-1' x=x+1 S95_t1(x)%id=2016071 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2016-071' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=13.3D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=260.0D0 S95_t1(x)%xmax=500.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='2016071_Atlas_gg-H-hh-WWgaga_13.3fb-1' x=x+1 S95_t1(x)%id=046702 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1509.04670 (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=20.3D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=260.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='04670_Atlas_H-hh-bbtautau_20.3fb-1' + x=x+1 + S95_t1(x)%id=336 + S95_t1(x)%particle_x=Hneut + S95_t1(x)%expt='ATL' + S95_t1(x)%label='[hep-ex] arXiv:1808.00336 (ATLAS)' + S95_t1(x)%energy=13.0D0 + S95_t1(x)%lumi=36.1D0 + S95_t1(x)%SMlike=0 + S95_t1(x)%xmin=260.0D0 + S95_t1(x)%xmax=1000.0D0 + S95_t1(x)%sep=5.0D0 + S95_t1(x)%deltax=10.0D0 + filename(x)='336_Atlas_X-HH-bbtautau_13TeV_36.1fb-1' + + x=x+1 S95_t1(x)%id=2016049 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATLAS' S95_t1(x)%label='ATLAS-CONF-2016-049' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=13.3D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=300.0D0 S95_t1(x)%xmax=3000.0D0 S95_t1(x)%sep=50.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='2016049_Atlas_H-hh-bbbb_13.3fb-1' x=x+1 S95_t1(x)%id=011811 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='[hep-ex] arXiv:1510.01181 (CMS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.7D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=260.0D0 S95_t1(x)%xmax=350.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='140341_CMS_H-hh-bbtautau_19.7fb-1' x=x+1 S95_t1(x)%id=17020321 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='[hep-ex] arXiv:1701.02032 (CMS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=5.0D0 S95_t1(x)%xmax=15.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='170102032_CMS_HSM-aa-tautau_19.7fb-1' x=x+1 S95_t1(x)%id=17020322 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='[hep-ex] arXiv:1701.02032 (CMS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=25.0D0 S95_t1(x)%xmax=62.5D0 S95_t1(x)%sep=0.5D0 S95_t1(x)%deltax=0.0D0 filename(x)='170102032_CMS_HSM-aa-mumubb_19.7fb-1' x=x+1 + S95_t1(x)%id=539 + S95_t1(x)%particle_x=Hneut + S95_t1(x)%expt='ATL' + S95_t1(x)%label='[hep-ex] arXiv:1807.00539 (ATLAS)' + S95_t1(x)%energy=13.0D0 + S95_t1(x)%lumi=36.1D0 + S95_t1(x)%SMlike=1 + S95_t1(x)%xmin=20.0D0 + S95_t1(x)%xmax=60.0D0 + S95_t1(x)%sep=0.5D0 + S95_t1(x)%deltax=0.0D0 + filename(x)='539_Atlas_H-aa-bbmumu_13TeV_36.1fb-1' + + x=x+1 S95_t1(x)%id=17020323 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='[hep-ex] arXiv:1701.02032 (CMS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=15.0D0 S95_t1(x)%xmax=62.5D0 S95_t1(x)%sep=0.5D0 S95_t1(x)%deltax=0.0D0 filename(x)='170102032_CMS_HSM-aa-mumutautau_19.7fb-1' x=x+1 S95_t1(x)%id=5051 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1509.05051 (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=20.3D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=10.0D0 S95_t1(x)%xmax=61.75D0 S95_t1(x)%sep=0.05D0 S95_t1(x)%deltax=0.0D0 filename(x)='5051_Atlas_gg-H-aa-gagagaga_20.3fb-1' x=x+1 S95_t1(x)%id=1506534 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='[hep-ex] arXiv:1510.06534 (CMS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.7D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=4.0D0 S95_t1(x)%xmax=8.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='1506534_CMS_gg-H-hh-tautautautau_19.7fb-1' x=x+1 S95_t1(x)%id=17006 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG 17-006' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=36.0D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=260.0D0 S95_t1(x)%xmax=900.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='17006_CMS_H-hh-bbVV-bblnulnu_36fb-1' x=x+1 S95_t1(x)%id=011812 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='[hep-ex] arXiv:1510.01181 (CMS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.7D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=220.0D0 S95_t1(x)%xmax=350.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='140342_CMS_A-hZ-tautaull_19.7fb-1' x=x+1 S95_t1(x)%id=044781 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATLAS' S95_t1(x)%label='[hep-ex] arXiv:1502.04478 (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=20.3D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=220.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='044781_ATLAS_gg-A-hZ-tautaull_20.3fb-1' x=x+1 S95_t1(x)%id=044782 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATLAS' S95_t1(x)%label='[hep-ex] arXiv:1502.04478 (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=20.3D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=220.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='044782_ATLAS_gg-A-hZ-bbll_20.3fb-1' x=x+1 S95_t1(x)%id=20160151 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATLAS' S95_t1(x)%label='ATLAS-CONF-2016-015' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=3.2D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=220.0D0 S95_t1(x)%xmax=2000.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='20160151_ATLAS_gg-A-hZ-bbll_3.2fb-1' x=x+1 S95_t1(x)%id=20160152 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATLAS' S95_t1(x)%label='ATLAS-CONF-2016-015' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=3.2D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=220.0D0 S95_t1(x)%xmax=2000.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='20160152_ATLAS_bb-A-hZ-bbll_3.2fb-1' x=x+1 S95_t1(x)%id=16002 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-16-002' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=2.3D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=260.0D0 S95_t1(x)%xmax=1200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='16002_CMS_H-hh-bbbb_2.3fb-1' ! x=x+1 ! S95_t1(x)%id=16029 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-16-029' ! S95_t1(x)%energy=13.0D0 ! S95_t1(x)%lumi=12.9D0 ! S95_t1(x)%SMlike=0 ! S95_t1(x)%xmin=250.0D0 ! S95_t1(x)%xmax=900.0D0 ! S95_t1(x)%sep=10.0D0 ! S95_t1(x)%deltax=10.0D0 ! filename(x)='16029_CMS_H-hh-bbtautau_12.9fb-1' x=x+1 S95_t1(x)%id=17002 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-17-002' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=35.9D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=250.0D0 S95_t1(x)%xmax=900.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='17002_CMS_H-hh-tautaubb_35.9fb-1' x=x+1 S95_t1(x)%id=14013 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-14-013,arXiv:1503.04114 (CMS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=17.9D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=270.0D0 S95_t1(x)%xmax=1097.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='14013_H-hh-bbbb_17.9fb-1' x=x+1 S95_t1(x)%id=17030 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-17-030' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=35.9D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=270.0D0 S95_t1(x)%xmax=3000.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='17030_CMS_pp-X-HH_comb_13TeV_35.9fb-1' !-------------------- H -> mu mu ------------------------- x=x+1 S95_t1(x)%id=2013010 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2013-010' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=21D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2013010_Atlas_H-mumu_21fb-1' x=x+1 S95_t1(x)%id=7663 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1406.7663 (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=24.8D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=120.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='7663_Atlas_H-mumu_24.8fb-1' !------------------------ H W -> W W W -------------------------- x=x+1 S95_t1(x)%id=5873 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 5873' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=3.6D0 S95_t1(x)%xmin=120.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=20.0D0 filename(x)='D0_WH_WWW_llnunu_3.6fb_5873' x=x+1 S95_t1(x)%id=7307 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='CDF Note 7307 vs 3' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=2.7D0 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=10.0D0 filename(x)='CDF_WH_WWW_2.7fb_7307vs3.0' !filename(x)='CDF_WH_WWW_1.9fb_7307' x=x+1 S95_t1(x)%id=1268 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='[hep-ex] arXiv:1107.1268 (D0)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=5.3D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=115.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_VH_ll_5.3fb_1268' ! x=x+1 ! S95_t1(x)%id=11034 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-034' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=4.6D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=115.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11034_CMS_WH-WWW_4.6fb-1_interpol' ! x=x+1 ! S95_t1(x)%id=12039 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-12-039' ! S95_t1(x)%energy=8.0D0 ! S95_t1(x)%lumi=10.D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='12039_CMS_WH-WWW_10fb-1' x=x+1 S95_t1(x)%id=13009 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-13-009' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=25.D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='13009_CMS_WH-WWW_25fb-1' x=x+1 S95_t1(x)%id=12006 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-12-006' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=4.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=140.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='12006_CMS_WH-Wtautau_4.7fb-1' x=x+1 S95_t1(x)%id=12051 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-12-051' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=17.D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=145.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='12051_CMS_VH_Vtautau_17fb-1' x=x+1 S95_t1(x)%id=2012078 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2012-078' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=4.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=300.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2012078_Atlas_WH_WWW_4.7fb-1' !-------------------- H -> gamma gamma -------------------- ! x=x+1 ! S95_t1(x)%id=6177 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 6177' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=8.2D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=2.5D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='D0_gaga_8.2fb_6177' x=x+1 S95_t1(x)%id=6295 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 6295' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=9.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=2.5D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_gaga_9.7fb_6295' x=x+1 S95_t1(x)%id=1887 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='[hep-ex] arXiv:0901.1887 (D0)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=2.7D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_Hgaga_2.7fb_1887' x=x+1 S95_t1(x)%id=10485 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='CDF Note 10485' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=7.0D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='CDF_SM_Hgaga_7.0fb_10485' x=x+1 S95_t1(x)%id=4960 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='TCB' S95_t1(x)%label='[hep-ex] arXiv:1107.4960 (TEVNPHWG)'!CDF Note 10510, D0 Note 6203 S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=8.2D0 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='CDF_D0_combined_SM_Hgaga_8.2fb_4960' x=x+1 S95_t1(x)%id=1414 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1202.1414 (ATLAS)' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=4.9D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='1414_Atlas_H-gaga_4.9fb-1' ! x=x+1 ! S95_t1(x)%id=2012091 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2012-091' ! S95_t1(x)%energy=8.0D0 ! S95_t1(x)%lumi=10.8D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=0.5D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2012091_Atlas_H-gaga_10.8fb-1' x=x+1 S95_t1(x)%id=2012168 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2012-168' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=17.8D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=0.5D0 S95_t1(x)%deltax=0.0D0 filename(x)='2012168_Atlas_H-gaga_17.8fb-1' x=x+1 S95_t1(x)%id=6583 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1407.6583' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=20.3D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=65.0D0 S95_t1(x)%xmax=600.0D0 S95_t1(x)%sep=0.1D0 S95_t1(x)%deltax=0.0D0 filename(x)='6583_Atlas_H-gaga_20.3fb-1' x=x+1 S95_t1(x)%id=059301 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1507.05930 (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=20.3D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=140.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='05930_Atlas_gg-H-ZZ-20.3fb-1' x=x+1 S95_t1(x)%id=059302 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1507.05930 (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=20.3D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=140.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='05930_Atlas_VBF-H-ZZ-20.3fb-1' x=x+1 S95_t1(x)%id=0038911 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1509.00389 (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=20.3D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=300.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=100.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='0038911_Atlas_ggH-WW-NWA_20.3fb-1' x=x+1 S95_t1(x)%id=0038912 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1509.00389 (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=20.3D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=300.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=100.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='0038912_Atlas_VBF-WW-NWA_20.3fb-1' x=x+1 S95_t1(x)%id=0038913 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1509.00389 (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=20.3D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=300.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=20.0D0 S95_t1(x)%deltax=20.0D0 filename(x)='0038913_Atlas_ggH-WW-CPS_20.3fb-1' x=x+1 S95_t1(x)%id=0038914 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1509.00389 (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=20.3D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=300.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=20.0D0 S95_t1(x)%deltax=20.0D0 filename(x)='0038914_Atlas_VBF-WW-CPS_20.3fb-1' + x=x+1 + S95_t1(x)%id=17013 + S95_t1(x)%particle_x=Hneut + S95_t1(x)%expt='CMS' + S95_t1(x)%label='CMS-PAS-HIG-17-013' + S95_t1(x)%energy=13.0D0 + S95_t1(x)%lumi=35.9D0 + S95_t1(x)%SMlike=1 + S95_t1(x)%xmin=80.0D0 + S95_t1(x)%xmax=110.0D0 + S95_t1(x)%sep=0.1D0 + S95_t1(x)%deltax=0.0D0 + filename(x)='17013_CMS_H-gaga_lowmass_8TeV_20fb-1_and_13TeV_36fb-1' + ! x=x+1 ! S95_t1(x)%id=1487 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='[hep-ex] arXiv:1202.1487 (CMS)' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=4.8D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=0.5D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='1487_CMS_H-gaga_4.8fb-1' ! x=x+1 ! S95_t1(x)%id=12001 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-12-001' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=4.76D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=0.5D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='12001_CMS_H-gaga_BDT_4.8fb-1' ! x=x+1 ! S95_t1(x)%id=12015 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-12-015' ! S95_t1(x)%energy=8.0D0 ! S95_t1(x)%lumi=9.9D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=0.5D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='12015_CMS_H-gaga_9.9fb-1' ! x=x+1 S95_t1(x)%id=13001 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-13-001' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=25.D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=0.5D0 S95_t1(x)%deltax=0.0D0 filename(x)='13001_CMS_H-gaga_MVA_25fb-1' x=x+1 S95_t1(x)%id=14037 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-14-037' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.7D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=80.0D0 S95_t1(x)%xmax=110.0D0 S95_t1(x)%sep=0.5D0 S95_t1(x)%deltax=0.0D0 filename(x)='14037_CMS_H-gaga_19.7fb-1' x=x+1 S95_t1(x)%id=14031 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-14-031' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.7D0 S95_t1(x)%SMlike=0 S95_t1(x)%xmin=200.0D0 S95_t1(x)%xmax=500.0D0 S95_t1(x)%sep=1.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='14031_CMS_H-Zgamma-19.7fb-1' + x=x+1 + S95_t1(x)%id=2018025 + S95_t1(x)%particle_x=Hneut + S95_t1(x)%expt='ATL' + S95_t1(x)%label='ATLAS-CONF-2018-025' + S95_t1(x)%energy=13.0D0 + S95_t1(x)%lumi=80.0D0 + S95_t1(x)%SMlike=0 + S95_t1(x)%xmin=65.0D0 + S95_t1(x)%xmax=110.0D0 + S95_t1(x)%sep=0.1D0 + S95_t1(x)%deltax=0.0D0 + filename(x)='2018025_Atlas_h-gaga_13TeV_80fb-1' + + ! x=x+1 ! S95_t1(x)%id=14006 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-14-006' ! S95_t1(x)%energy=8.0D0 ! S95_t1(x)%lumi=19.7D0 ! S95_t1(x)%SMlike=0 ! S95_t1(x)%xmin=150.0D0 ! S95_t1(x)%xmax=847.6D0 ! S95_t1(x)%sep=0.1D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='14006_CMS_H-gaga_19.7fb-1' ! !-------------------- H -> gamma Z -------------------- ! x=x+1 ! S95_t1(x)%id=13006 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-13-006' ! S95_t1(x)%energy=8.0D0 ! S95_t1(x)%lumi=25.D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=120.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=1.D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='13006_CMS_H-gaZ_25fb-1' x=x+1 S95_t1(x)%id=13075515 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='[hep-ex] arXiv:1307.5515 (CMS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=24.6D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=120.0D0 S95_t1(x)%xmax=160.0D0 S95_t1(x)%sep=0.1D0 S95_t1(x)%deltax=0.0D0 filename(x)='13075515_CMS_H-Zgamma_24.6fb-1' ! x=x+1 ! S95_t1(x)%id=2013009 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2013-009' ! S95_t1(x)%energy=8.0D0 ! S95_t1(x)%lumi=25.D0 ! S95_t1(x)%SMlike=1 ! S95_t1(x)%xmin=120.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=1.D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2013009_Atlas_H-gaZ_25fb-1' x=x+1 S95_t1(x)%id=3051 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1402.3051 (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=24.8D0 S95_t1(x)%SMlike=1 S95_t1(x)%xmin=120.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=0.1D0 S95_t1(x)%deltax=0.0D0 filename(x)='3051_Atlas_H-Zga_24.8fb-1' !--------------------- b H -> b tau tau --------------------------- x=x+1 S95_t1(x)%id=4885 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='[hep-ex] arXiv:1106.4885 (D0)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=7.3D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=320.0D0 S95_t1(x)%sep=10.0D0 filename(x)='D0_Hb_tautaub_7.3fb_4885' ! x=x+1 ! S95_t1(x)%id=5985 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 5985' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=2.7D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=320.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='D0_bH_btautau_2.7fb_5985' ! x=x+1 ! S95_t1(x)%id=5974 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 5974' ! S95_t1(x)%energy=1.96D0 ! S95_t1(x)%lumi=3.7D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=300.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='D0_Hb_tautaub_3.7fb_5974' x=x+1 S95_t1(x)%id=6083 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 6083' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=4.3D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=200.0D0 S95_t1(x)%sep=10.0D0 filename(x)='D0_Hb_tautaub_4.3fb_6083' !-------------------- t t H -> t t b b -------------------- x=x+1 S95_t1(x)%id=5739 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='D0 Note 5739' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=2.1D0 S95_t1(x)%xmin=105.0D0 S95_t1(x)%xmax=155.0D0 S95_t1(x)%sep=10.0D0 filename(x)='D0_ttH_ttbb_2.1fb_5739' x=x+1 S95_t1(x)%id=10574 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CDF' S95_t1(x)%label='CDF Note 10574' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=7.5D0 S95_t1(x)%xmin=100.0D0 S95_t1(x)%xmax=170.0D0 S95_t1(x)%sep=5.0D0 filename(x)='CDF_ttH_ttbb_7.5fb_10574_interpol' x=x+1 S95_t1(x)%id=2012135 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2012-135' S95_t1(x)%energy=7D0 S95_t1(x)%lumi=4.7D0 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=140.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2012135_Atlas_ttH_Hbb_4.7fb-1' x=x+1 S95_t1(x)%id=12025 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-12-025' S95_t1(x)%energy=7D0 S95_t1(x)%lumi=5.D0 S95_t1(x)%xmin=110.0D0 S95_t1(x)%xmax=140.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='12025_CMS_ttH-ttbb_5fb-1' !-------------------- H -> Z gamma -------------------------- x=x+1 S95_t1(x)%id=0611 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt=' D0' S95_t1(x)%label='[hep-ex] arXiv:0806.0611 (D0)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=1.1D0 S95_t1(x)%xmin=120.0D0 S95_t1(x)%xmax=320.0D0 S95_t1(x)%sep=20.0D0 filename(x)='D0_H-Zgamma_1.0-1.1fb_0611' !x=x+1 !S95_t1(x)%id=6091 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 6091' !S95_t1(x)%xmin=115.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='D0_VH_ll_5.4fb_6091' !x=x+1 !S95_t1(x)%id=5858 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 5858' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=2.5D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='D0_gaga_4.2fb_5858' !x=x+1 !S95_t1(x)%id=10065 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 10065' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=10.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='CDF_SM_Hgaga_5.4fb_10065' ! x=x+1 ! S95_t1(x)%id=0968 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='[hep-ex] arXiv:0912.0968 (D0)' ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=320.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='D0_Hb_tautaub_2.7fb_0968' !---------------- Daniel's attempts -------------- x=x+1 S95_t1(x)%id=2016025 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-HIG-16-025' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=2.69D0 S95_t1(x)%xmin=550.0D0 S95_t1(x)%xmax=1200.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='2016025_CMS_H-bb_2.69fb-1' x=x+1 S95_t1(x)%id=201608391 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATLAS' S95_t1(x)%label='ATLAS-1606-08391' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=3.2D0 S95_t1(x)%xmin=20.0D0 S95_t1(x)%xmax=60.0D0 S95_t1(x)%sep=0.5D0 S95_t1(x)%deltax=10.0D0 filename(x)='160608391_Atlas_HW_Waa_Wbbbb_3.2fb-1' x=x+1 S95_t1(x)%id=2016044 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATLAS' S95_t1(x)%label='ATLAS-CONF-2016-044' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=13.3D0 S95_t1(x)%xmin=250.0D0 S95_t1(x)%xmax=2500.0D0 S95_t1(x)%sep=2D0 S95_t1(x)%deltax=10.0D0 filename(x)='2016044_Atlas_H_ZA_13.3fb-1' x=x+1 S95_t1(x)%id=2016004 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATLAS' S95_t1(x)%label='ATLAS-CONF-2016-004' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=3.2D0 S95_t1(x)%xmin=275.0D0 S95_t1(x)%xmax=400.0D0 S95_t1(x)%sep=1D0 S95_t1(x)%deltax=10.0D0 filename(x)='2016004_Atlas_H-hh-bbgaga_3.2fb-1' x=x+1 S95_t1(x)%id=1604833 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATLAS' S95_t1(x)%label='ATLAS-1606-04833' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=3.2D0 S95_t1(x)%xmin=500.0D0 S95_t1(x)%xmax=3000.0D0 S95_t1(x)%sep=10D0 S95_t1(x)%deltax=10.0D0 filename(x)='1604833_Atlas_H-VV_3.2fb-1' x=x+1 S95_t1(x)%id=2016056 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATLAS' S95_t1(x)%label='ATLAS-CONF-2016-056' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=13.3D0 S95_t1(x)%xmin=300.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=5D0 S95_t1(x)%deltax=10.0D0 filename(x)='2016056_Atlas_H-ZZ-llnunu_13.3fb-1' x=x+1 S95_t1(x)%id=20160551 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATLAS' S95_t1(x)%label='ATLAS-CONF-2016-055' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=15.5D0 S95_t1(x)%xmin=1200.0D0 S95_t1(x)%xmax=3000.0D0 S95_t1(x)%sep=100D0 S95_t1(x)%deltax=10.0D0 filename(x)='20160551_Atlas_pp-H-ZZ-qqqq_15.5fb-1' x=x+1 S95_t1(x)%id=20160552 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='ATLAS' S95_t1(x)%label='ATLAS-CONF-2016-055' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=15.5D0 S95_t1(x)%xmin=1200.0D0 S95_t1(x)%xmax=3000.0D0 S95_t1(x)%sep=100D0 S95_t1(x)%deltax=10.0D0 filename(x)='20160552_Atlas_pp-H-WW-qqqq_15.5fb-1' x=x+1 S95_t1(x)%id=15009 S95_t1(x)%particle_x=Hneut S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-2015-009' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.7D0 S95_t1(x)%xmin=25.0D0 S95_t1(x)%xmax=60.0D0 S95_t1(x)%sep=0.1D0 S95_t1(x)%deltax=1.0D0 filename(x)='15009_CMS_bbA_mumu_19.7fb-1' !---------------- charged Higgs ------------------ x=x+1 S95_t1(x)%id=1811 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt=' D0' S95_t1(x)%label='[hep-ex] arXiv:0908.1811 (D0)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=1.0D0 S95_t1(x)%xmin=80.0D0 S95_t1(x)%xmax=155.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_Hp_qq_1.0fb_1811_interpol' x=x+1 S95_t1(x)%id=1269 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='CDF' S95_t1(x)%label='[hep-ex] arXiv:0907.1269 (CDF) lower mass' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=2.2D0 S95_t1(x)%xmin=60.0D0 S95_t1(x)%xmax=70.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='CDF_t-Hplusb_1269_lowmass' x=x+1 S95_t1(x)%id=1270 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='CDF' S95_t1(x)%label='[hep-ex] arXiv:0907.1269 (CDF) higher mass' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=2.2D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='CDF_t-Hplusb_1269_highmass' x=x+1 S95_t1(x)%id=7712 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='CDF' S95_t1(x)%label='CDF Note 7712' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=0.192D0 S95_t1(x)%xmin=80.0D0 S95_t1(x)%xmax=160.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='CDF_t-Hplusb_tauonicHM_192pb_7712' x=x+1 S95_t1(x)%id=8353 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='CDF' S95_t1(x)%label='CDF Note 8353' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=0.335D0 S95_t1(x)%xmin=80.0D0 S95_t1(x)%xmax=120.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='CDF_t-Hplusb_8353' x=x+1 S95_t1(x)%id=1812 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt=' D0' S95_t1(x)%label='[hep-ex] arXiv:0908.1811 (D0)' S95_t1(x)%energy=1.96D0 S95_t1(x)%lumi=1.0D0 S95_t1(x)%xmin=80.0D0 S95_t1(x)%xmax=155.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='D0_Hp_taunu_1.0fb_1811_interpol' x=x+1 S95_t1(x)%id=2011094 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2011-094' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=0.035D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=130.0D0 S95_t1(x)%sep=20.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2011094_Atlas_Hplus-cs_35pb-1' ! x=x+1 ! S95_t1(x)%id=2011138 ! S95_t1(x)%particle_x=Hplus ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2011-138' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=1.03D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=160.0D0 ! S95_t1(x)%sep=10.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2011138_Atlas_Hp-taunu_1.03fb-1' ! x=x+1 ! S95_t1(x)%id=2011151 ! S95_t1(x)%particle_x=Hplus ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2011-151' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=1.03D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=160.0D0 ! S95_t1(x)%sep=10.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2011151_Atlas_chargedH-taunu_1.03fb-1' x=x+1 S95_t1(x)%id=2760 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1204.2760 (ATLAS)' S95_t1(x)%energy=7.0D0 S95_t1(x)%lumi=4.6D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=160.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2760_Atlas_Hp_taunu_4.6fb-1' ! x=x+1 ! S95_t1(x)%id=2013090 ! S95_t1(x)%particle_x=Hplus ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2013-090' ! S95_t1(x)%energy=8.0D0 ! S95_t1(x)%lumi=19.5D0 ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=160.0D0 ! S95_t1(x)%sep=10.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2013090_Atlas_Hp_taunu_19.6fb-1' x=x+1 S95_t1(x)%id=2014050 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2014-050' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.5D0 S95_t1(x)%xmin=80.0D0 S95_t1(x)%xmax=160.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2014050_Atlas_Hp_taunu_19.5fb-1' x=x+1 S95_t1(x)%id=79151 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1807.07915 (ATLAS)' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=36.1D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=2000.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='079151_Atlas_tbHp-taunu_36fb-1' x=x+1 S95_t1(x)%id=79152 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='ATL' S95_t1(x)%label='[hep-ex] arXiv:1807.07915 (ATLAS)' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=36.1D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=160.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='079152_Atlas_t-Hpb-taunu_36fb-1' ! x=x+1 ! S95_t1(x)%id=11008 ! S95_t1(x)%particle_x=Hplus ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-008' ! S95_t1(x)%energy=7.0D0 ! S95_t1(x)%lumi=1.1D0 ! S95_t1(x)%xmin=80.0D0 ! S95_t1(x)%xmax=160.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11008_CMS_Hplus-taunu_1.1fb-1_interpol' x=x+1 S95_t1(x)%id=14020 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-14-020' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.7D0 S95_t1(x)%xmin=80.0D0 S95_t1(x)%xmax=160.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='14020_CMS_Hp_taunu_19.7fb-1' x=x+1 S95_t1(x)%id=13035 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-13-035' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.7D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=160.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='13035_CMS_chargedH-cs_19.7fb-1' x=x+1 S95_t1(x)%id=16030 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-16-030' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=19.7D0 S95_t1(x)%xmin=90.0D0 S95_t1(x)%xmax=150.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='16030_CMS_t_Hplusb_cb_19.7fb-1' ! HB-5 x=x+1 S95_t1(x)%id=1504233 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='ATLAS' S95_t1(x)%label='arXiv:1503.04233 [hep-ex] (ATLAS)' S95_t1(x)%energy=8.0D0 S95_t1(x)%lumi=20.3D0 S95_t1(x)%xmin=200.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=20.0D0 S95_t1(x)%deltax=10.0D0 filename(x)='1504233_Atlas_Hplus_VBF-WZ_20.3fb-1' x=x+1 S95_t1(x)%id=160312 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-16-031' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=12.9D0 S95_t1(x)%xmin=180.0D0 S95_t1(x)%xmax=3000.0D0 S95_t1(x)%sep=10.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='16031_CMS_Hptb_taunu_12.9fb-1' x=x+1 S95_t1(x)%id=160311 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='CMS' S95_t1(x)%label='CMS-PAS-HIG-16-031' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=12.9D0 S95_t1(x)%xmin=80.0D0 S95_t1(x)%xmax=160.0D0 S95_t1(x)%sep=5.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='160311_CMS_t_Hplusb_taunu_12.9fb-1' x=x+1 S95_t1(x)%id=2016088 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2016-088' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=14.7D0 S95_t1(x)%xmin=200.0D0 S95_t1(x)%xmax=2000.0D0 S95_t1(x)%sep=25.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2016088_Atlas_Hptb-taunutb_14.7fb-1' x=x+1 S95_t1(x)%id=2016089 S95_t1(x)%particle_x=Hplus S95_t1(x)%expt='ATL' S95_t1(x)%label='ATLAS-CONF-2016-089' S95_t1(x)%energy=13.0D0 S95_t1(x)%lumi=13.2D0 S95_t1(x)%xmin=300.0D0 S95_t1(x)%xmax=1000.0D0 S95_t1(x)%sep=50.0D0 S95_t1(x)%deltax=0.0D0 filename(x)='2016089_Atlas_Hptb-tbtb_13.2fb-1' !---------------------------------------------- !&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&& ! superseded !x=x+1 !superseded by arXiv:1011.1931 !S95_t1(x)%id=3556 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='[hep-ex] arXiv:0805.3556 (D0)' !S95_t1(x)%xmin=90.0D0 !S95_t1(x)%xmax=220.0D0 !S95_t1(x)%sep=10.0D0 !filename(x)='D0_bbH_bb_1.0fb_3556_interpol' !x=x+1 !superseded by arXiv:1009.3047 !S95_t1(x)%id=3534 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='[hep-ex] arXiv:0908.3534 (CDF)' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='CDF_ZH_llbb_2.7fb_3534' !x=x+1 !superseded by CDF 10239 !S95_t1(x)%id=10217 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 10217' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='CDF_WH_lnubb_5.6fb_10217' !x=x+1 !superseded by CDF Note 10133 !S95_t1(x)%id=9248 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 9248' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='CDF_SMcomb_tautau_2.0fb_9248_interpol' !x=x+1 !superseded by arXiv:1012.0874 !S95_t1(x)%id=1970 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='[hep-ex] arXiv:0808.1970 (D0)' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='D0_WH_lnubb_1.05fb_1970' !x=x+1 !S95_t1(x)%id=6095 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 6095' !S95_t1(x)%xmin=115.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='D0_H-WW_lljj_5.4fb_6095' !x=x+1 !S95_t1(x)%id=5972 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 5972' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='D0_WH_lnubb_5.0fb_5972' !x=x+1 !S95_t1(x)%id=10068 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 10068' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='CDF_WH_lnubb_4.8fb_10068' !x=x+1 !S95_t1(x)%id=5586 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 5586' !S95_t1(x)%xmin=105.0D0 !S95_t1(x)%xmax=145.0D0 !S95_t1(x)%sep=10.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='D0_ZH_nunubb_2.1fb_5586' !x=x+1 !S95_t1(x)%id=9891 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 9891' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='CDF_VH_Metbb_3.6fb_9891' !x=x+1 !S95_t1(x)%id=5876 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 5876' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='D0_ZH_llbb_4.2fb_5876' !x=x+1 !S95_t1(x)%id=9889 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 9889' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='CDF_ZH_llbb_4.1fb_9889' !x=x+1 !S95_t1(x)%id=9284 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 9284' !S95_t1(x)%xmin=90.0D0 !S95_t1(x)%xmax=210.0D0 !S95_t1(x)%sep=10.0D0 !filename(x)='CDF_bbH_bb_1.9fb_9284' !x=x+1 !S95_t1(x)%id=9868 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 9868' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='CDF_WH_lnubb_4.3fb_9868' !http://www-cdf.fnal.gov/physics/new/hdg/results/whlnubb_090814/WH4.3fb.html !x=x+1 !S95_t1(x)%id=9887 !superseded by arXiv:1001.4468 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 9887' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='CDF_H-WW_4.8fb_9887_interpol' !x=x+1 !S95_t1(x)%id=0024 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='[hep-ex] arXiv:0811.0024v1 (D0)' !S95_t1(x)%xmin=90.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=10.0D0 !filename(x)='D0_bH_btautau_328pb_0024' !x=x+1 !S95_t1(x)%id=1266 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='[hep-ex] arXiv:0808.1266 (D0)' !S95_t1(x)%xmin=105.0D0 !S95_t1(x)%xmax=135.0D0 !S95_t1(x)%sep=10.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='D0_VH_bb_0.93fb_1266' !x=x+1 !S95_t1(x)%id=0432 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='[hep-ex] arXiv:0802.0432 (CDF)' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=140.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='CDF_VH_Metbb_1fb_0432' !x=x+1 !S95_t1(x)%id=9674 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 9674' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='CDF_SM_combined_2.0-3.0fb_9674_interpol' !x=x+1 !S95_t1(x)%id=5980 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='TCB' !S95_t1(x)%label='D0 Note 5980, CDF Note 9888' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=10.0D0 !filename(x)='CDF_D0_combinedH-tautau_2.2fb_5980' !x=x+1 !S95_t1(x)%id=9714 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='TCB' !S95_t1(x)%label='arXiv:0903.4001 (TEVNPHWG), MH>=155GeV'!CDF Note 9713, D0 Note 5889 !S95_t1(x)%xmin=155.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='CDF_D0_SM_combined_4.2fb_9713-5889_bayesian_highmassonly' !x=x+1 !S95_t1(x)%id=9897 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 9897' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='CDF_SM_combined_2.0-4.8fb_9897_interpol' !x=x+1 !S95_t1(x)%id=8742 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 8742' ! table from CDF note 8742 !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='CDF_ZH_llbb_1fb_8742_interpol' ! x=x+1 ! S95_t1(x)%id=7081 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CDF' ! S95_t1(x)%label='arxiv 070810 (CDF)' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='CDF_ZH_nunubb_1.7fb_070810_interpol' ! ! x=x+1 ! ! S95_t1(x)%id=8958 ! ! S95_t1(x)%particle_x=Hneut ! ! S95_t1(x)%expt='CDF' ! ! S95_t1(x)%label='CDF Note 8958' ! ! S95_t1(x)%xmin=110.0D0 ! ! S95_t1(x)%xmax=200.0D0 ! ! S95_t1(x)%sep=10.0D0 ! ! filename(x)='CDF_ggH_WW_1.9fb_8958' ! x=x+1 ! S95_t1(x)%id=8957 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CDF' ! S95_t1(x)%label='CDF Note 8957' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! filename(x)='CDF_WH_lnubb_1.7fb_8957_interpol' ! x=x+1 ! S95_t1(x)%id=5489 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 5489' ! S95_t1(x)%xmin=120.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=20.0D0 ! filename(x)='D0_ppH_WW_emu_0.6fb_5489' !x=x+1 !S95_t1(x)%id=5537 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 5537' !S95_t1(x)%xmin=120.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=20.0D0 !filename(x)='D0_ppH_WW_ll_1.7fb_5537' ! x=x+1 ! S95_t1(x)%id=5482 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 5482' ! S95_t1(x)%xmin=105.0D0 ! S95_t1(x)%xmax=145.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='D0_ZH_llbb_1.1fb_5482' ! x=x+1 ! S95_t1(x)%id=5624 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 5624' ! S95_t1(x)%xmin=115.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! filename(x)='D0_ppH_WW_ll_2.3fb_5624' !x=x+1 !S95_t1(x)%id=5472 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 5472' !S95_t1(x)%xmin=105.0D0 !S95_t1(x)%xmax=145.0D0 !S95_t1(x)%sep=10.0D0 !!filename(x)='D0_WH_lnubb_1.7fb_5472' !filename(x)='D0_WH_lnubb_1.7fb_5472_Fig.6a' !x=x+1 !S95_t1(x)%id=5502 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 5502' !S95_t1(x)%xmin=120.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=20.0D0 !filename(x)='D0_ppH_WW_ee_0.6fb_5502' !x=x+1 !S95_t1(x)%id=5332 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 5332' !S95_t1(x)%xmin=120.0D0 !S95_t1(x)%xmax=180.0D0 !S95_t1(x)%sep=20.0D0 !filename(x)='D0_ppH_WW_mutau_1fb_5332' !x=x+1 !S95_t1(x)%id=5485 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 5485' !S95_t1(x)%xmin=120.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=20.0D0 !filename(x)='D0_WH_WWW_llnunu_1fb_5485' !x=x+1 !S95_t1(x)%id=9071 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 9071' !S95_t1(x)%xmin=90.0D0 !S95_t1(x)%xmax=250.0D0 !S95_t1(x)%sep=10.0D0 !filename(x)='CDF_ppH_tautau_1.8fb_9071_interpol' !x=x+1 !S95_t1(x)%id=5331 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 5331' !S95_t1(x)%xmin=90.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=10.0D0 !filename(x)='D0_ppH_tautau_1fb_5331_interpol' ! x=x+1 ! S95_t1(x)%id=5503 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 5503' ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=170.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='D0_bbH_bb_0.9fb_5503_interpol' !x=x+1 !S95_t1(x)%id=8954 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 8954' !S95_t1(x)%xmin=90.0D0 !S95_t1(x)%xmax=210.0D0 !S95_t1(x)%sep=10.0D0 !filename(x)='CDF_bbH_bb_1fb_8954' ! x=x+1 ! S95_t1(x)%id=9236 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CDF' ! S95_t1(x)%label='CDF Note 9236' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='CDF_ggH_WW_2.4fb_9236' ! x=x+1 ! S95_t1(x)%id=9219 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CDF' ! S95_t1(x)%label='CDF Note 9219' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! filename(x)='CDF_WH_lnubb_1.9fb_9219' ! x=x+1 ! S95_t1(x)%id=5601 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 5601' ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='D0_Hgaga_2.27fb_5601' !taken out until we sort out a fermiophobic-ness test !x=x+1 !S95_t1(x)%id=1514 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='[hep-ex] arXiv:0803.1514v1 (D0)' !S95_t1(x)%xmin=70.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=10.0D0 !filename(x)='D0_gaga_1.1fb_1514' ! x=x+1 ! S95_t1(x)%id=9166 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CDF' ! S95_t1(x)%label='CDF Note 9166' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='CDF_VH_Metbb_1.97fb_9166_interpol' !x=x+1 !S95_t1(x)%id=9463 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 9463' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='CDF_WH_lnubb_2.7fb_9463' !x=x+1 !S95_t1(x)%id=5570 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 5570' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='D0_ZH_llbb_2.3fb_5570' !x=x+1 !S95_t1(x)%id=4493 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='[hep-ex] arXiv:0807.4493 (CDF)' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='CDF_ZH_llbb_1fb_4493_interpol' !x=x+1 !S95_t1(x)%id=9475 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 9475' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='CDF_ZH_llbb_2.4fb_9475' !x=x+1 !S95_t1(x)%id=5737 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 5737' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='D0_gaga_2.68fb_5737' !x=x+1 !S95_t1(x)%id=9483 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF note 9483' !S95_t1(x)%xmin=105.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='CDF_VH_Metbb_2.1fb_9483' !x=x+1 !S95_t1(x)%id=9500 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 9500' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='CDF_ggH_WW_3.0fb_9500_interpol' !x=x+1 !S95_t1(x)%id=9713 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='TCB' !S95_t1(x)%label='CDF Note 9713, D0 Note 5889' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='CDF_D0_SM_combined_4.2fb_9713-5889_bayesian' ! x=x+1 ! S95_t1(x)%id=1024 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CDF' ! S95_t1(x)%label='CDF Note XXXX, zhllbb_081024' ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! filename(x)='CDF_ZH_llbb_2.7fb_1024' !x=x+1 !S95_t1(x)%id=9596 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 9596' !S95_t1(x)%xmin=100.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='CDF_WH_lnubb_2.7fb_9596' ! x=x+1 ! S95_t1(x)%id=5828 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 5828' ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! filename(x)='D0_WH_lnubb_2.7fb_5828' !x=x+1 !S95_t1(x)%id=9642 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 9642' !S95_t1(x)%xmin=105.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='CDF_VH_Metbb_2.1fb_9642' ! x=x+1 ! S95_t1(x)%id=9022 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CDF' ! S95_t1(x)%label='CDF Note 9764,"old" ggH XS' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='CDF_H-WW_3.6fb_9022_interpol' !NEW! not yet in OB's code !x=x+1 !S95_t1(x)%id=9023 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 9764,"new" ggH XS' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 !filename(x)='CDF_H-WW_3.6fb_9023_interpol' ! x=x+1 ! S95_t1(x)%id=3493 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CDF' ! S95_t1(x)%label='[hep-ex] arXiv:0803.3493v1 (CDF)' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! filename(x)='CDF_WH_lnubb_1fb_3493_interpol' !x=x+1 !S95_t1(x)%id=0710 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note XXXX,hwwmenn_090710' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='CDF_H-WW_4.8fb_0710_interpol' !x=x+1 !S95_t1(x)%id=5984 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 5984,high mass' !S95_t1(x)%xmin=155.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='D0_SM_combined_5984_highmassonly' !x=x+1 !S95_t1(x)%id=3155 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='[hep-ex] arXiv:0905.3155 (CDF)' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='CDF_WH_lnubb_1.9fb_3155_interpol' ! x=x+1 ! S95_t1(x)%id=9997 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='TCB' ! S95_t1(x)%label='arXiv:0911.3930 (TEVNPHWG), MH>=160GeV'!CDF Note 9998, D0 Note 5983 ! S95_t1(x)%xmin=160.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='CDF_D0_SM_combined_2.1-5.4fb_9998-5983_bayesian_highmassonly' !x=x+1 !S95_t1(x)%id=6039 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='TCB' !S95_t1(x)%label='CDF Note 10101, D0 Note 6039' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=260.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='CDF_D0_combined_gg-H-WW_4.8-5.4fb_6039_bayesian_interpol' !x=x+1 !S95_t1(x)%id=6006 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt=' D0' !S95_t1(x)%label='D0 Note 6006' !S95_t1(x)%xmin=115.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='D0_H-WW_ll_5.4fb_6006' !x=x+1 !S95_t1(x)%id=2011026 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='ATL' !S95_t1(x)%label='ATLAS-CONF-2011-026' !S95_t1(x)%xmin=200.0D0 !S95_t1(x)%xmax=600.0D0 !S95_t1(x)%sep=20.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='2011026_Atlas_H-VV_35pb-1' !x=x+1 !superseded by 2011085 !S95_t1(x)%id=2011025 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='ATL' !S95_t1(x)%label='ATLAS-CONF-2011-025' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=140.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='2011025_Atlas_H-gaga_37.6pb-1_interpol' !x=x+1 !S95_t1(x)%id=2011005 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='ATL' !S95_t1(x)%label='ATLAS-CONF-2011-005' !S95_t1(x)%xmin=120.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='2011005_Atlas_H-WW_35pb-1_interpol' !x=x+1 !S95_t1(x)%id=10433 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 10432' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=300.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='CDF_ggH-WW_7.1fb_10433_SMnormalized' !x=x+1 !S95_t1(x)%id=10432 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='CDF' !S95_t1(x)%label='CDF Note 10432' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=200.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='CDF_H-WW_7.1fb_10432' ! x=x+1 ! S95_t1(x)%id=6170 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 6170' ! S95_t1(x)%xmin=100.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='D0_ZH_bb_6.2fb_6170' ! x=x+1 ! S95_t1(x)%id=6182 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 6182' ! S95_t1(x)%xmin=115.0D0 ! S95_t1(x)%xmax=200.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='D0_H-VV_8.1fb_6182' !x=x+1 superseded by 2011131 !S95_t1(x)%id=2011048 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='ATL' !S95_t1(x)%label='ATLAS-CONF-2011-048' !S95_t1(x)%xmin=120.0D0 !S95_t1(x)%xmax=600.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='2011048_Atlas_H-ZZ-4l_40pb-1_interpol' !x=x+1 !S95_t1(x)%id=2011085 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='ATL' !S95_t1(x)%label='ATLAS-CONF-2011-085' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=140.0D0 !S95_t1(x)%sep=1.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='2011085_Atlas_H-gaga_209pb-1' ! x=x+1 ! S95_t1(x)%id=2748 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='[hep-ex] arXiv:1106.2748 (ATLAS)' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2748_Atlas_SMcombined_40pb-1' !x=x+1 !S95_t1(x)%id=11002 !S95_t1(x)%particle_x=Hplus !S95_t1(x)%expt='CMS' !S95_t1(x)%label='CMS-PAS-HIG-11-002' !S95_t1(x)%xmin=80.0D0 !S95_t1(x)%xmax=160.0D0 !S95_t1(x)%sep=5.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='11002_CMS_t-Hplusb_36pb-1' !x=x+1 !S95_t1(x)%id=2011020 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='ATL' !S95_t1(x)%label='ATLAS-CONF-2011-020, lower masses' !S95_t1(x)%xmin=6.1D0 !S95_t1(x)%xmax=9.0D0 !S95_t1(x)%sep=0.1D0 !filename(x)='2011020_Atlas_H-mumu_lowerMa_35pb-1' !x=x+1 !S95_t1(x)%id=2011021 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='ATL' !S95_t1(x)%label='ATLAS-CONF-2011-020, higher masses' !S95_t1(x)%xmin=11.0D0 !S95_t1(x)%xmax=11.9D0 !S95_t1(x)%sep=0.1D0 !filename(x)='2011021_Atlas_H-mumu_higherMa_35pb-1' ! x=x+1 ! S95_t1(x)%id=11003 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-003' ! S95_t1(x)%xmin=115.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11003_CMS_H-WW_1.1fb-1_interpol' ! x=x+1 ! S95_t1(x)%id=11004 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-004' ! S95_t1(x)%xmin=120.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=10.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11004_CMS_H-ZZ-llll_1.13fb-1' ! x=x+1 ! S95_t1(x)%id=11005 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-005' ! S95_t1(x)%xmin=250.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=10.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11005_CMS_H-ZZ-llnunu_1.1fb-1' ! x=x+1 ! S95_t1(x)%id=11006 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-006' ! S95_t1(x)%xmin=230.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11006_CMS_H-ZZ-llqq_1fb-1' ! x=x+1 ! S95_t1(x)%id=11009 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-009' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=140.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11009_CMS_SM_H-tautau_1.1fb-1' ! x=x+1 ! S95_t1(x)%id=11010 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-010' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=140.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11010_CMS_H-gammagamma_1.09fb-1' !x=x+1 !S95_t1(x)%id=2011111 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='ATL' !S95_t1(x)%label='ATLAS-CONF-2011-111' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=240.0D0 !S95_t1(x)%sep=5.0D0 !filename(x)='2011111_Atlas_H-WW_1.04fb-1_interpol' !x=x+1 !S95_t1(x)%id=2011131 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='ATL' !S95_t1(x)%label='ATLAS-CONF-2011-131' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=600.0D0 !S95_t1(x)%sep=2.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='2011131_Atlas_H-ZZ_1.1fb-1_interpol' ! x=x+1 ! S95_t1(x)%id=11012 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-012' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=135.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11012_CMS_H-bb_1.1fb-1' ! x=x+1 ! S95_t1(x)%id=11013 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-013' ! S95_t1(x)%xmin=180.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=10.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11013_CMS_H-ZZ-lltautau_1.1fb-1' ! x=x+1 ! S95_t1(x)%id=11014 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-014' ! S95_t1(x)%xmin=115.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11014_CMS_H-WW_1.55fb-1_interpol' ! x=x+1 ! S95_t1(x)%id=11015 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-015' ! S95_t1(x)%xmin=115.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11015_CMS_H-ZZ-4l_1.66fb-1_interpol' ! x=x+1 ! S95_t1(x)%id=11016 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-016' ! S95_t1(x)%xmin=250.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11016_CMS_H-ZZ-llnunu_1.6fb-1_interpol' ! x=x+1 ! S95_t1(x)%id=11017 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-017' ! S95_t1(x)%xmin=225.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11017_CMS_H-ZZ-llqq_1.6fb-1_interpol' ! x=x+1 ! S95_t1(x)%id=11020 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-020' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=145.0D0 ! S95_t1(x)%sep=5.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11020_CMS_H-tautau_1.6fb-1_SM' ! x=x+1 ! S95_t1(x)%id=11021 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-021' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11021_CMS_SM_H-gaga_1.66fb-1' !n.b.: Need fermiophobic-ness check for this analysis ! x=x+1 ! S95_t1(x)%id=110212 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-021' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='110212_CMS_Fermiophob_H-gaga_1.66fb-1' ! x=x+1 ! S95_t1(x)%id=11022 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-022' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11022_CMS_SMcombined_1.1-1.7fb-1' ! x=x+1 ! S95_t1(x)%id=5895 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='[hep-ex] arXiv:1108.5895 (ATLAS)' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='5895_Atlas_H-gaga_1.08fb-1' ! x=x+1 ! S95_t1(x)%id=110201 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-020' ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=500.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='11020_CMS_H-tautau_1.6fb-1_MSSM_interpol' !x=x+1 !S95_t1(x)%id=2011161 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='ATL' !S95_t1(x)%label='ATLAS-CONF-2011-161' !S95_t1(x)%xmin=110.0D0 !S95_t1(x)%xmax=150.0D0 !S95_t1(x)%sep=1.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='2011161_Atlas_H-gaga_4.9fb-1' ! x=x+1 ! S95_t1(x)%id=2011162 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='ATL' ! S95_t1(x)%label='ATLAS-CONF-2011-162' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='2011162_Atlas_H-ZZ-4l_4.8fb-1' ! x=x+1 ! S95_t1(x)%id=11024 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-024' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=5D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11024_CMS_H-WW-lnulnu_4.6fb-1_interpol' ! x=x+1 ! S95_t1(x)%id=11025 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-025' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11025_CMS_H-ZZ-4l_4.7fb-1' ! x=x+1 ! S95_t1(x)%id=11026 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-026' ! S95_t1(x)%xmin=250.0D0 ! S95_t1(x)%xmax=590.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11026_CMS_H-ZZ-llnunu_4.6fb-1' ! x=x+1 ! S95_t1(x)%id=110271 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-027' ! S95_t1(x)%xmin=130.0D0 ! S95_t1(x)%xmax=164.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='110271_CMS_H-ZZ-llqq_4.6fb-1' ! x=x+1 ! S95_t1(x)%id=110272 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-027' ! S95_t1(x)%xmin=200.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='110272_CMS_H-ZZ-llqq_4.6fb-1' ! x=x+1 ! S95_t1(x)%id=11028 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-028' ! S95_t1(x)%xmin=190.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11028_CMS_H-ZZ-lltautau_4.7fb-1' ! x=x+1 ! S95_t1(x)%id=11030 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-030' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=150.0D0 ! S95_t1(x)%sep=0.5D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11030_CMS_H-gaga_4.8fb-1' ! x=x+1 ! S95_t1(x)%id=11032 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt='CMS' ! S95_t1(x)%label='CMS-PAS-HIG-11-032' ! S95_t1(x)%xmin=110.0D0 ! S95_t1(x)%xmax=600.0D0 ! S95_t1(x)%sep=1.0D0 ! S95_t1(x)%deltax=0.0D0 ! filename(x)='11032_CMS_SMcombined_4.7fb-1' !x=x+1 !S95_t1(x)%id=2011150 !S95_t1(x)%particle_x=Hneut !S95_t1(x)%expt='ATL' !S95_t1(x)%label='ATLAS-CONF-2011-150' !S95_t1(x)%xmin=200.0D0 !S95_t1(x)%xmax=600.0D0 !S95_t1(x)%sep=20.0D0 !S95_t1(x)%deltax=0.0D0 !filename(x)='2011150_Atlas_H-ZZ-llqq_2.05fb-1' ! x=x+1 ! S95_t1(x)%id=6224 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 6227, Br(h->tautau)>6%' ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=300.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='D0_h-bb_h-tautau_comb_Br0.06_5.2-7.3fb_6224' ! ! x=x+1 ! S95_t1(x)%id=6225 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 6227, Br(h->tautau)>10%' ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=300.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='D0_h-bb_h-tautau_comb_Br0.10_5.2-7.3fb_6225' ! ! x=x+1 ! S95_t1(x)%id=6226 ! S95_t1(x)%particle_x=Hneut ! S95_t1(x)%expt=' D0' ! S95_t1(x)%label='D0 Note 6227, Br(h->tautau)>14%' ! S95_t1(x)%xmin=90.0D0 ! S95_t1(x)%xmax=300.0D0 ! S95_t1(x)%sep=10.0D0 ! filename(x)='D0_h-bb_h-tautau_comb_Br0.14_5.2-7.3fb_6226' ! checks we've filled the whole array if(x.ne.xend)then stop 'error in initializetables1 (a)' endif ! do loop to read in S95 tables col=3 do x=xbeg,xend S95_t1(x)%nx=nint((S95_t1(x)%xmax-S95_t1(x)%xmin)/S95_t1(x)%sep)+1 allocate(S95_t1(x)%dat(S95_t1(x)%nx,col-1)) enddo open(file_id_common2,file = trim(adjustl(pathname))//'Expt_tables/' // & & 'S95_t1.binary',form='unformatted') read(file_id_common2,iostat=ios)S95_t1(xbeg)%dat if(ios.eq.0)then do x=xbeg+1,xend read(file_id_common2)S95_t1(x)%dat enddo else rewind(file_id_common2) do x=xbeg,xend fullfilename=trim(adjustl(pathname))//'Expt_tables/' & & //trim(adjustl(S95_t1(x)%expt))//'tables/' & & //trim(filename(x))//'.txt' call read_tabletype1(S95_t1(x),5,col,fullfilename) #ifndef WEBVERSION write(file_id_common2)S95_t1(x)%dat #endif enddo endif close(file_id_common2) deallocate(filename) end subroutine initializetables1 !************************************************************ subroutine read_tabletype1(t1,skip,col,fullfilename) !************************************************************ !fills t1%dat !--------------------------------------input type(table1) :: t1 integer :: skip,col character(LEN=*) :: fullfilename !-----------------------------------internal integer :: i,n double precision :: xdummy,xdummy_store !------------------------------------------- t1%dat=0.0D0 open(file_id_1, file=(trim(fullfilename))) do i=1,skip read(file_id_1,*) !skip lines enddo xdummy_store = t1%xmin-t1%sep do i=1,t1%nx read(file_id_1,*)xdummy,(t1%dat(i,n),n=1,col-1) ! if(minval(t1%dat(i,:)).lt.0) then ! write(*,*) xdummy,minval(t1%dat(i,:)) ! endif ! checks that x are evenly spaced as expected if((abs(xdummy-xdummy_store-t1%sep).gt.1.0D-7) & & .or.(abs(xdummy-(t1%xmin+dble(i-1)*t1%sep)).gt.1.0D-7))then write(*,*)i,t1%id,xdummy,t1%xmin+dble(i-1)*t1%sep stop 'error in read_tabletype1 (a1)' endif xdummy_store=xdummy enddo if(abs(xdummy-t1%xmax).gt.1.0D-7)stop 'error in read_tabletype1 (a2)' close(file_id_1) end subroutine read_tabletype1 !************************************************************ end module S95tables_type1 !************************************************************