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minipaper.tex

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HiggsBounds\cite{arXiv:0811.4169,arXiv:1102.1898} version 3.1.0beta uses the following experimental analyses: \cite{arXiv:0911.3930,arXiv:1011.1931,arXiv:1103.3233,arXiv:0912.0968,hep-ex/0206022,arXiv:0805.2491,arXiv:0906.1014,arXiv:1008.3564,arXiv:1005.3216,hep-ex/0107032,arXiv:0911.3935,arXiv:1001.4468,hep-ex/0401022,arXiv:0712.0598,arXiv:0912.5285,arXiv:0707.0373,hep-ex/0107031,arXiv:0907.1269,arXiv:0806.0611,arXiv:0905.3381,arXiv:1003.3363,hep-ex/0111010,arXiv:0804.3423,arXiv:1009.3047,hep-ex/0501033,arXiv:1012.0874,arXiv:0808.0534,arXiv:1001.4162,arXiv:0809.3930,hep-ex/0602042,arXiv:0906.5613,arXiv:0908.1811,arXiv:0712.2383,arXiv:1007.4587,arXiv:0903.4800,hep-ex/0404012,arXiv:1001.4481,arXiv:0901.1887,hep-ex/0410017,CDFnotes,D0notes,CMSnotes,ATLASnotes,LHWGnotes}
.
Internally, {\tt HiggsBounds} uses a number of Standard Model results for the Higgs sector\cite{hep-ph/9704448,hep-ph/0102227,hep-ph/0102241,hep-ph/0201206,hep-ph/0207004,hep-ph/0302135,arXiv:0811.3458,Dawson:1990zj,Djouadi:1991tka,hep-ph/9504378,hep-ph/0404071,hep-ph/0407249,arXiv:0809.1301,arXiv:0809.3667,hep-ph/0306211,arXiv:0901.2427,hep-ph/0307206,hep-ph/0306234,hep-ph/0406152,hep-ph/0304035,hep-ph/9206246,hep-ph/9905386,hep-ph/0306109,hep-ph/0403194,hep-ph/0612172,hep-ph/0107081,hep-ph/0107101,hep-ph/0211438,hep-ph/0305321,arXiv:0705.2744,arXiv:0707.0381,arXiv:0710.4749,arXiv:1101.0593,hep-ph/0304035}
to convert between experimental limits with different normalisations.
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