{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.76843.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1444991"}},{"@id":"https://doi.org/10.1007/JHEP08(2016)104","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2017","description":"CERN-LHC. This paper describes a measurement of fiducial and differential cross sections of gluon-fusion Higgs boson production in the H->WW*->e nu mu nu channel, using 20.3 fb^{-1} of proton--proton collision data. The data were produced at a centre-of-mass energy of sqrt(s) = 8 TeV at the CERN Large Hadron Collider and recorded by the ATLAS detector in 2012.  Cross sections are measured from the observed H->WW*->e nu mu nu signal yield in categories distinguished by the number of associated jets. The total cross section is measured in a fiducial region defined by the kinematic properties of the charged leptons and neutrinos. Differential cross sections are reported as a function of the number of jets, the Higgs boson transverse momentum, the dilepton rapidity, and the transverse momentum of the leading jet.  The jet-veto efficiency, or fraction of events with no jets above a given transverse momentum threshold, is also reported.  All measurements are compared to QCD predictions from Monte Carlo generators and fixed-order calculations, and are in agreement with the Standard Model predictions.\n\nThe fiducial region is defined as:\n- 1 electron, 1 muon, 2 neutrinos, n jets\n- electron: pT> 15 GeV, |eta|< 1.37 or 1.52< |eta|< 2.47\n- muon: pT> 15 GeV, |eta|< 2.5\n- jets: pT> 25 GeV if |eta|< 2.4, pT> 30 GeV if 2.4 <|eta|< 4.5\n- leading lepton: pT> 22 GeV\n- 10 < M(e,mu) < 55 GeV\n- Delta_Phi(e,mu) < 1.8\n- missing transeverse momentum > 20 GeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t1","@type":"Dataset","description":"Measured total fiducial cross section in fb.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t2","@type":"Dataset","description":"Measured fiducial cross section in fb as a function of Njet. Jet PT>25 GeV for |eta|<2.4 and PT>30 GeV for...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t3","@type":"Dataset","description":"Measured fiducial cross section in fb/GeV as a function of pTH.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t4","@type":"Dataset","description":"Measured fiducial cross section in fb as a function of Yll.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t5","@type":"Dataset","description":"Measured fiducial cross section in fb/GeV as a function of the leading jet pT, PT(JET1).","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t6","@type":"Dataset","description":"Measured normalised fiducial cross section as a function of Njet. Jet PT>25 GeV for |eta|<2.4 and PT>30 GeV for 2.4<|eta|<4.5.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t7","@type":"Dataset","description":"Measured normalised fiducial cross section in 1/GeV as a function of pTH.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t8","@type":"Dataset","description":"Measured normalised fiducial cross section as a function of Yll.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t9","@type":"Dataset","description":"Measured normalised fiducial cross section in 1/GeV as a function of the leading jet pT, PT(JET1).","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t10","@type":"Dataset","description":"Jet veto efficiency as a function of PT(JET1) pT threshold.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t11","@type":"Dataset","description":"Full correlation matrix for the measured differential cross section as a function of Njet, taking into account statistical and systematic...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t12","@type":"Dataset","description":"Full correlation matrix for the measured differential cross section as a function of pTH, taking into account statistical and systematic...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t13","@type":"Dataset","description":"Full correlation matrix for the measured differential cross section as a function of Yll, taking into account statistical and systematic...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t14","@type":"Dataset","description":"Full correlation matrix for the measured differential cross section as a function of the leading jet pT, taking into account...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t15","@type":"Dataset","description":"Full correlation matrix for the measured normalised differential cross section as a function of Njet, taking into account statistical and...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t16","@type":"Dataset","description":"Full correlation matrix for the measured normalised differential cross section as a function of pTH, taking into account statistical and...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t17","@type":"Dataset","description":"Full correlation matrix for the measured normalised differential cross section as a function of Yll, taking into account statistical and...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t18","@type":"Dataset","description":"Full correlation matrix for the measured normalised differential cross section as a function of the leading jet pT, taking into...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t19","@type":"Dataset","description":"Fiducial cross section of H+0-jet events in femtobarn for different values of PT(JET1) pT threshold with the uncertainties for each...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t20","@type":"Dataset","description":"Correction factors from inclusive parton level to fiducial particle level for bins of Njet derived with POWHEG NNLOPS+Pythia8. Uncertainties due...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t21","@type":"Dataset","description":"Correction factors from inclusive parton level to fiducial particle level for bins of the leading jet pT derived with POWHEG...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.76843.v1/t22","@type":"Dataset","description":"Correction factors from inclusive parton level to fiducial particle level for the jet-veto efficiency with different jet pT thresholds derived...","name":"Table 22"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1444991?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/76843"}],"inLanguage":"en","name":"Measurement of fiducial differential cross sections of gluon-fusion production of Higgs bosons decaying to $WW^{\\ast}{\\rightarrow\\,}e\\nu\\mu\\nu$ with the ATLAS detector at $\\sqrt{s}=8$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1444991?version=1","version":1}