{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.115994.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2014187"}},{"@id":"https://doi.org/10.1007/JHEP08(2022)175","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2022","description":"Measurements of the production cross-sections of the Standard Model (SM) Higgs boson ($H$) decaying into a pair of $\\tau$-leptons are presented.  The measurements use data collected with the ATLAS detector from $pp$ collisions produced at the Large Hadron Collider at a centre-of-mass energy of $\\sqrt{s}$=13TeV, corresponding to an integrated luminosity of 139 fb$^{-1}$. Leptonic ($\\tau\\rightarrow l \\nu_{l}\\nu_{\\tau}$) and hadronic ($\\tau\\rightarrow$ hadrons $\\nu_{\\tau}$ ) decays of the $\\tau$-lepton are considered.  All measurements account for the branching ratio of $H\\rightarrow\\tau\\tau$ and are performed with a requirement $|y_{H}|<2.5$, where $y_{H}$ is the true Higgs boson rapidity. The cross-section of the pp$\\rightarrow H\\rightarrow \\tau\\tau $ process is measured to be $2.94 \\pm 0.21$ (stat) $^{+0.37}_{-0.32}$ (syst) pb, in agreement with the SM predictions $ 3.17 \\pm 0.09$ pb. Inclusive cross-sections are determined separately for the four dominant production mode, $2.65 \\pm 0.41$ (stat) $^{+0.91}_{-0.67}$ (syst) pb for gluon-gluon fusion, $ 0.197 \\pm 0.028 $ (stat) $^{+0.032}_{-0.026}$ (syst) pb for vector-boson fusion, $ 0.115 \\pm 0.058 $ (stat) $^{+0.042}_{-0.040} $ (syst) pb for vector-boson associated production and $ 0.033 \\pm 0.031 $ (stat) $^{+0.022}_{-0.017}$ (syst) pb for top-quark pair associated production. Measurements in exclusive regions of the phase space, using the simplified template cross-section framework, are also performed.  All results are in agreement with the SM predictions.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t1","@type":"Dataset","description":"Observed yields in the boost_0_1J signal region category of the hh channel.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t2","@type":"Dataset","description":"Observed yields in the boost_0_ge2J signal region category of the hh channel.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t3","@type":"Dataset","description":"Observed yields in the boost_1_1J signal region category of the hh channel.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t4","@type":"Dataset","description":"Observed yields in the boost_1_ge2J signal region category of the hh channel.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t5","@type":"Dataset","description":"Observed yields in the boost_2 signal region category of the hh channel.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t6","@type":"Dataset","description":"Observed yields in the boost_3 signal region category of the hh channel.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t7","@type":"Dataset","description":"Observed yields in the ttH_0 signal region category of the hh channel.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t8","@type":"Dataset","description":"Observed yields in the ttH_1 signal region category of the hh channel.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t9","@type":"Dataset","description":"Observed yields in the VH_0 signal region category of the hh channel.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t10","@type":"Dataset","description":"Observed yields in the VH_1 signal region category of the hh channel.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t11","@type":"Dataset","description":"Observed yields in the VBF_0 signal region category of the hh channel.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t12","@type":"Dataset","description":"Observed yields in the VBF_1 signal region category of the hh channel.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t13","@type":"Dataset","description":"Observed yields in the boost_0_1J signal region category of the lh channel.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t14","@type":"Dataset","description":"Observed yields in the boost_0_ge2J signal region category of the lh channel.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t15","@type":"Dataset","description":"Observed yields in the boost_1_1J signal region category of the lh channel.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t16","@type":"Dataset","description":"Observed yields in the boost_1_ge2J signal region category of the lh channel.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t17","@type":"Dataset","description":"Observed yields in the boost_2 signal region category of the lh channel.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t18","@type":"Dataset","description":"Observed yields in the boost_3 signal region category of the lh channel.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t19","@type":"Dataset","description":"Observed yields in the VH_0 signal region category of the lh channel.","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t20","@type":"Dataset","description":"Observed yields in the VH_1 signal region category of the lh channel.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t21","@type":"Dataset","description":"Observed yields in the VBF_0 signal region category of the lh channel.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t22","@type":"Dataset","description":"Observed yields in the VBF_1 signal region category of the lh channel.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t23","@type":"Dataset","description":"Observed yields in the boost_0_1J signal region category of the ll channel.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t24","@type":"Dataset","description":"Observed yields in the boost_0_ge2J signal region category of the ll channel.","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t25","@type":"Dataset","description":"Observed yields in the boost_1_1J signal region category of the ll channel.","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t26","@type":"Dataset","description":"Observed yields in the boost_1_ge2J signal region category of the ll channel.","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t27","@type":"Dataset","description":"Observed yields in the boost_2 signal region category of the ll channel.","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t28","@type":"Dataset","description":"Observed yields in the boost_3 signal region category of the ll channel.","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t29","@type":"Dataset","description":"Observed yields in the VH_0 signal region category of the ll channel.","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t30","@type":"Dataset","description":"Observed yields in the VH_1 signal region category of the ll channel.","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t31","@type":"Dataset","description":"Observed yields in the VBF_0 signal region category of the ll channel.","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t32","@type":"Dataset","description":"Observed yields in the VBF_1 signal region category of the ll channel.","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t33","@type":"Dataset","description":"Best-fit values and uncertainties for the pp $\\rightarrow H\\rightarrow\\tau\\tau$ cross-section measurement and the measurement in the four dominant production modes....","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t34","@type":"Dataset","description":"The measured correlations between each parameter of interest in the measurement of the cross-sections per production mode","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t35","@type":"Dataset","description":"Best-fit values and uncertainties for the $H\\rightarrow\\tau\\tau$ cross-sections, in the reduced stage 1.2 STXS scheme. The EW production mode includes...","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.115994.v2/t36","@type":"Dataset","description":"The measured correlations between each pair of parameters of interest in the STXS measurement. The asterisk symbol (*) indicates that...","name":"Table 36"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2014187?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/115994"}],"inLanguage":"en","name":"Measurements of Higgs boson production cross-sections in the $H\\to\\tau^{+}\\tau^{-}$ decay channel in $pp$ collisions at $\\sqrt{s}=13\\,\\text{TeV}$ with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2014187?version=2","version":2}