diff --git a/analyses/pluginCMS/CMS_2018_I1653948.info b/analyses/pluginCMS/CMS_2018_I1653948.info --- a/analyses/pluginCMS/CMS_2018_I1653948.info +++ b/analyses/pluginCMS/CMS_2018_I1653948.info @@ -1,44 +1,48 @@ Name: CMS_2018_I1653948 Year: 2018 Summary: Measurement of the inelastic proton-proton cross section at 13 TeV Experiment: CMS Collider: LHC InspireID: 1653948 Status: VALIDATED Authors: + - cms-pag-conveners-smp@cern.ch - Sercan Sen - Pierre Van Mechelen - Hans Van Haevermaet References: + - JHEP 07 (2018) 161 + - DOI 10.1007/JHEP07(2018)161 - CMS-FSQ-15-005 + - arXiv:1802.02613 [hep-ex] - CERN-EP-2018-004 - - ARXIV:1802.02613 [hep-ex] + - http://cms-results.web.cern.ch/cms-results/public-results/publications/FSQ-15-005/ RunInfo: Inelastic events (non-diffractive and inelastic diffractive). NumEvents: 1M Beams: [p+, p+] Energies: [13000] PtCuts: Description: 'A measurement of the inelastic proton-proton cross section at $\sqrt{s} = 13$ TeV with the CMS detector at the LHC has been presented. An inelastic cross section of $67.5 \pm 0.8 \text{(syst)} \pm 1.6 \text{(lumi)}$ mb is obtained for $\xi = M^2/s > 10^{-6}$ (corresponding to $M > 13$ GeV), with $M$ the larger of $M_{\mathrm{X}}$ and $M_{\mathrm{Y}}$, where $M_{\mathrm{X}}$ and $M_{\mathrm{Y}}$ are the masses of the diffractive dissociation systems with negative and positive pseudorapidities, respectively. In addition, an inelastic cross section of $68.6 \pm 0.5 \text{(syst)} \pm 1.6 \text{(lumi)}$ mb is obtained in the enlarged phase space $\xi_{\mathrm{X}} > 10^{-7}$ and/or $\xi_{\mathrm{Y}} > 10^{-6}$ (corresponding to $M_{\mathrm{X}} > 4.1$ GeV and/or $M_{\mathrm{Y}} > 13$ GeV).' BibKey: Sirunyan:2018nqx BibTeX: '@article{Sirunyan:2018nqx, author = "Sirunyan, Albert M and others", title = "{Measurement of the inelastic proton-proton cross section at $\sqrt{s}=$ 13 TeV}", collaboration = "CMS", year = "2018", eprint = "1802.02613", archivePrefix = "arXiv", primaryClass = "hep-ex", reportNumber = "CMS-FSQ-15-005, CERN-EP-2018-004", SLACcitation = "%%CITATION = ARXIV:1802.02613;%%" }' diff --git a/analyses/pluginCMS/CMS_2018_I1680318.info b/analyses/pluginCMS/CMS_2018_I1680318.info --- a/analyses/pluginCMS/CMS_2018_I1680318.info +++ b/analyses/pluginCMS/CMS_2018_I1680318.info @@ -1,48 +1,51 @@ Name: CMS_2018_I1680318 Year: 2018 Summary: Charged particle distributions in different final states at 13~TeV Experiment: CMS collaboration Collider: LHC InspireID: 1680318 Status: VALIDATED Authors: + - cms-pag-conveners-smp@cern.ch - Juan Manuel Grados Luyando - Pieters Maxim References: - - arXiv:1806.11245 - - CMS-FSQ-16-011 - Eur.Phys.J. C78 (2018) no.9, 697 + - DOI: 10.1140/epjc/s10052-018-6144-y + - arXiv:1806.11245 [hep-ex] + - inspirehep: 1680318 + - http://cms-results.web.cern.ch/cms-results/public-results/publications/FSQ-16-011/ RunInfo: 'Inelastic events at 13~TeV centre of mass energy. Tracks in $|\eta|<2.4$ and with $\pT > 0.5~GeV$' #NumEvents: 10000000 NeedCrossSection: no Beams: [p+, p+] Energies: [13000] Description: 'Charged particle distributions in different final states at $\sqrt{s} = 13$~TeV by the CMS experiment. Pseudorapidity, multiplicity and transverse momentum distributions of all charged particles. Also the $\pT$ leading charged particle spectrum and its integration as function of $\pT$. The distributions are presented for inelastic, non-single-diffractive and single-diffractive event selections. Please note, that the MC predictions are not scaled to the datapoints, in contrast to Figure 6 in the publication.' BibKey: Sirunyan:2018zdc BibTeX: '@article{Sirunyan:2018zdc, author = "Sirunyan, Albert M. and others", title = "{Measurement of charged particle spectra in minimum-bias - events from proton–proton collisions at + events from proton-proton collisions at $\sqrt{s}=13\,\text {TeV} $}", collaboration = "CMS", journal = "Eur. Phys. J.", volume = "C78", year = "2018", number = "9", pages = "697", doi = "10.1140/epjc/s10052-018-6144-y", eprint = "1806.11245", archivePrefix = "arXiv", primaryClass = "hep-ex", reportNumber = "CMS-FSQ-16-011, CERN-EP-2018-187", SLACcitation = "%%CITATION = ARXIV:1806.11245;%%" }' diff --git a/analyses/pluginCMS/CMS_2018_I1682495.info b/analyses/pluginCMS/CMS_2018_I1682495.info --- a/analyses/pluginCMS/CMS_2018_I1682495.info +++ b/analyses/pluginCMS/CMS_2018_I1682495.info @@ -1,39 +1,42 @@ Name: CMS_2018_I1682495 Year: 2018 Summary: Jet mass in dijet events in $pp$ collisions at 13~TeV Experiment: CMS Collider: LHC SpiresID: 1682495 Status: VALIDATED Authors: + - cms-pag-conveners-smp@cern.ch - Salvatore Rappoccio References: + - JHEP 11 (2018) 113 + - DOI 10.1007/JHEP11(2018)113 - hep-ex arXiv:1807.05974 - inspirehep 1682495 - http://cms-results.web.cern.ch/cms-results/public-results/publications/SMP-16-010/index.html RunInfo: $pp$ QCD interactions at $\sqrt{s} = 13$ TeV. Data collected by CMS during the year 2015. Beams: [p+, p+] Energies: [13000] PtCuts: [200] NeedCrossSection: yes Description: 'Measurements of the differential jet cross section are presented as a function of jet mass in dijet events, in bins of jet transverse momentum, with and without a jet grooming algorithm. The data have been recorded by the CMS Collaboration in proton-proton collisions at the LHC at a center-of-mass energy of 13\TeV and correspond to an integrated luminosity of 2.3\fbinv. The absolute cross sections show slightly different jet transverse momentum spectra in data and Monte Carlo event generators for the settings used. Removing this transverse momentum dependence, the normalized cross section for ungroomed jets is consistent with the prediction from Monte Carlo event generators for masses below 30\% of the transverse momentum. The normalized cross section for groomed jets is measured with higher precision than the ungroomed cross section. Semi-analytical calculations of the jet mass beyond leading logarithmic accuracy are compared to data, as well as predictions at leading order and next-to-leading order, which include parton showering and hadronization. Overall, in the normalized cross section, the theoretical predictions agree with the measured cross sections within the uncertainties for masses from 10 to 30\% of the jet transverse momentum.'