{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.102525.v4","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1850544"}},{"@id":"https://doi.org/10.1140/epjc/s10052-021-09200-x","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2022","description":"CERN-LHC. Production cross sections of the Higgs boson are measured in the the H to ZZ to 4l (l= e, \u03bc) decay channel. A data sample of proton-proton collisions at a center-of-mass energy of 13 TeV, collected by the CMS detector at the LHC and corresponding to an integrated luminosity of 137 /fb is used. The signal strength modifier \u03bc, defined as the ratio of the Higgs boson production rate in the 4\u2113 channel to the standard model (SM) expectation, is measured to be \u03bc = 0.94 \u00b1 0.07 (stat) \u22120.08 / +0.09 (syst) at a fixed value of mH = 125.38 GeV. The signal strength modifiers for the individual Higgs boson production modes are also reported. The inclusive fiducial cross section for the H \u2192 4\u2113 process is measured to be 2.84 \u22120.22 / +0.23  (stat) \u22120.21 / +0.26 (syst) fb, which is compatible with the SM prediction of 2.84 \u00b1 0.15 fb for the same fiducial region. Differential cross sections as a function of the transverse momentum and rapidity of the Higgs boson, the number of associated jets, and the transverse momentum of the leading associated jet are measured. A new set of cross section measurements in mutually exclusive categories targeted to identify production mechanisms and kinematical features of the events is presented. The results are in agreement with the SM predictions.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.102525.v4/t1","@type":"Dataset","description":"Integrated Fiducial Higgs cross section. The first uncertainty is the combined statistical uncertainty, the second is the combined systematic uncertainty....","name":"Fiducial HZZ cross section: function of center-of-mass energy"},{"@id":"https://doi.org/10.17182/hepdata.102525.v4/t2","@type":"Dataset","description":"Integrated Fiducial Higgs cross section individually with 2016, 2017 and 2018 dataset and with full Run 2 dataset. The first...","name":"Fiducial HZZ cross section per year"},{"@id":"https://doi.org/10.17182/hepdata.102525.v4/t3","@type":"Dataset","description":"Higgs fiducial cross section in bins of pT for the 4 leptons. The first uncertainty is statistical, the second is...","name":"Fiducial differential HZZ cross section in pT(H) bins"},{"@id":"https://doi.org/10.17182/hepdata.102525.v4/t4","@type":"Dataset","description":"Higgs fiducial cross section in bins of rapidity for the 4 leptons. The first uncertainty is statistical, the second is...","name":"Fiducial differential HZZ cross section in |y(H)| bins"},{"@id":"https://doi.org/10.17182/hepdata.102525.v4/t5","@type":"Dataset","description":"Higgs fiducial cross section in bins of Jet Multiplicity The first uncertainty is statistical, the second is systematic uncertainty.","name":"Fiducial differential HZZ cross section in Njets bins"},{"@id":"https://doi.org/10.17182/hepdata.102525.v4/t6","@type":"Dataset","description":"Higgs fiducial cross section in bins of pT of leading jet. The first uncertainty is statistical, the second is the...","name":"Fiducial differential HZZ cross section in pT(lead. jet) bins"},{"@id":"https://doi.org/10.17182/hepdata.102525.v4/t7","@type":"Dataset","description":"Results of likelihood scans for the signal strength modifiers corresponding to the five main SM H boson production mechanisms. The...","name":"Signal strengths"},{"@id":"https://doi.org/10.17182/hepdata.102525.v4/t8","@type":"Dataset","description":"Result of the 2D likelihood scan for the bosonic and fermionic signal strength modifiers. Contour for the 68% CL region.","name":"Fermionic and bosonic signal strengths: 68% CL"},{"@id":"https://doi.org/10.17182/hepdata.102525.v4/t9","@type":"Dataset","description":"Result of the 2D likelihood scan for the bosonic and fermionic signal strength modifiers. Contour for the 95% CL region.","name":"Fermionic and bosonic signal strengths: 95% CL"},{"@id":"https://doi.org/10.17182/hepdata.102525.v4/t10","@type":"Dataset","description":"The measured product of cross section times branching fraction for HZZ decay and the SM predictions for the Stage 0...","name":"STXS Stage 0 cross sections"},{"@id":"https://doi.org/10.17182/hepdata.102525.v4/t11","@type":"Dataset","description":"The measured product of cross section times branching fraction for HZZ decay and the SM predictions for the merged Stage...","name":"STXS Stage 1.2 cross sections"},{"@id":"https://doi.org/10.17182/hepdata.102525.v4/t12","@type":"Dataset","description":"Observed correlation matrix between the measured cross sections for the Stage 0 for HZZ decay.","name":"Correlations: STXS Stage 0 cross sections"},{"@id":"https://doi.org/10.17182/hepdata.102525.v4/t13","@type":"Dataset","description":"Observed correlation matrix between the measured cross sections for the Stage 1.2 for HZZ decay.","name":"Correlations: STXS Stage 1.2 cross sections"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1850544?version=4"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/102525"}],"inLanguage":"en","name":"Measurements of production cross sections of the Higgs boson in the four-lepton final state in proton-proton collisions at $\\sqrt{s} = $ 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1850544?version=4","version":4}