{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.105961.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1894790"}},{"@id":"https://doi.org/10.1103/PhysRevLett.128.081805","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2021","description":"CERN-LHC.The cross section for Higgs boson production in pp collisions is studied using the H -> TAU + TAU - decay mode. The measurements are performed using data collected by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb^-1 . The Higgs boson transverse momentum (pT) is reconstructed using the visible tau decay products and missing pT. The jets are defined in accordance with STXS jet definition. The differential cross section times branching fraction is measured as a function of the Higgs boson pT, jet multiplicity, and pT of the leading jet, in a fiducial phase space defined to match the experimental acceptance in terms of the lepton kinematics and event topology. Results are unfolded to particle level.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.105961.v1/t1","@type":"Dataset","description":"The fiducial differential signal strength and cross section in each Higgs pT bin. Both the unregularized and regularized signal strengths...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.105961.v1/t2","@type":"Dataset","description":"The fiducial differential signal strength and cross section in each jet multiplicity bin. Both the unregularized and regularized signal strengths...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.105961.v1/t3","@type":"Dataset","description":"The fiducial differential signal strength and cross section in each leading jet pT bin. Both the unregularized and regularized signal...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.105961.v1/t4","@type":"Dataset","description":"The correlation matrix for the Higgs pT measurements, both for the unregularized and regularized fits. The last bin is inclusive.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.105961.v1/t5","@type":"Dataset","description":"The correlation matrix for the jet multiplicity measurements, both for the unregularized and regularized fits. The last bin is inclusive.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.105961.v1/t6","@type":"Dataset","description":"The correlation matrix for the leading jet pT measurements, both for the unregularized and regularized fits. The last bin is...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.105961.v1/t7","@type":"Dataset","description":"The fiducial integrated signal strength and cross section.","name":"Table 7"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1894790?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/105961"}],"inLanguage":"en","name":"Measurement of the inclusive and differential Higgs boson production cross sections in the decay mode to a pair of $\\tau$ leptons in pp collisions at $\\sqrt{s} = $ 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1894790?version=1","version":1}