{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.93071.v4","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1782650"}},{"@id":"https://doi.org/10.1103/PhysRevLett.125.051801","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2020","description":"CERN-LHC. A search for additional heavy neutral Higgs bosons is performed using a data sample corresponding to an integrated luminosity of 139 fb$^{-1}$ from proton-proton collisions at $\\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC.\n\nThe 1l1tau_h channel fiducial region is defined as:\n- 1e+>=1tau_h or 1mu+>=1tau_h\n- ptLepton > 30 GeV\n- |etaMuon| < 2.4, |etaEle| < 2.47 (excluding 1.37 < |etaEle| < 1.52)\n- ptTauVis > 25 GeV\n- |etaTauVis| < 2.3 (excluding 1.37 < |etaTauVis| < 1.52)\n- No events with more than 1 electron (ptEle > 15 GeV) or muon (ptMuon > 7 GeV, |etaMuon|<2.5)\n- If multiple tau_h exist, the leading visible pt one is chosen\n- l and tau_h opposite electric charge\n- |DeltaPhi(l,tau_h)| > 2.4 rad\n- mT(l,MET) < 40 GeV\n- veto 80 < m(l,tau_h) < 110 in 1e1tau_h channel\n\nThe 2tau_h channel fiducial region is defined as:\n- >=2tau_h\n- ptTauVis > 65 GeV (at least one with ptTauVis > 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)\n- No events with an electron or muon, ptLepton > 7 (15) GeV for muons (electrons), |etaMuon| < 2.5, |etaEle| < 2.47 (excluding 1.37 < |etaEle| < 1.52)\n- If more than two tau_h exist, the two leading visible pt ones are chosen\n- The two tau_h have opposite electric charge\n- |DeltaPhi(tau1_h,tau2_h)| > 2.7 rad\n\nFor Higgs interpretations events entering the fiducial region of each channel are categorised as: \n- \"b-tag: if they contain a b-quark initiated jet (ptJet > 20 GeV, |etaJet|<2.5)\"\n- \"b-veto: otherwise\"","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t1","@type":"Dataset","description":"Observed and predicted mTtot distribution in the b-veto category of the 1l1tau_h channel. Please note that the bin content is...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t2","@type":"Dataset","description":"Observed and predicted mTtot distribution in the b-tag category of the 1l1tau_h channel. Please note that the bin content is...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t3","@type":"Dataset","description":"Observed and predicted mTtot distribution in the b-veto category of the 2tau_h channel. Please note that the bin content is...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t4","@type":"Dataset","description":"Observed and predicted mTtot distribution in the b-tag category of the 2tau_h channel. Please note that the bin content is...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t5","@type":"Dataset","description":"Observed and expected 95% CL upper limits on the gluon-gluon fusion Higgs boson production cross section times ditau branching fraction...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t6","@type":"Dataset","description":"Observed and expected 95% CL upper limits on the b-associated Higgs boson production cross section times ditau branching fraction as...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t7","@type":"Dataset","description":"The observed 95% CL upper limits on $\\tan\\beta$ as a function of $m_{A}$ in the $M_{h}^{125}$ scenario. The lowest value...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t8","@type":"Dataset","description":"The expected 95% CL upper limits on $\\tan\\beta$ as a function of $m_{A}$ in the $M_{h}^{125}$ scenario. The lowest value...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t9","@type":"Dataset","description":"The expected 95% CL upper limits with plus one sigma on $\\tan\\beta$ as a function of $m_{A}$ in the $M_{h}^{125}$...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t10","@type":"Dataset","description":"The expected 95% CL upper limits with minus one sigma on $\\tan\\beta$ as a function of $m_{A}$ in the $M_{h}^{125}$...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t11","@type":"Dataset","description":"The expected 95% CL upper limits with plus two sigma on $\\tan\\beta$ as a function of $m_{A}$ in the $M_{h}^{125}$...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t12","@type":"Dataset","description":"The expected 95% CL upper limits with minus two sigma on $\\tan\\beta$ as a function of $m_{A}$ in the $M_{h}^{125}$...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t13","@type":"Dataset","description":"The observed 95% CL upper limits on $\\tan\\beta$ as a function of $m_{A}$ in the hMSSM scenario. The lowest value...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t14","@type":"Dataset","description":"The expected 95% CL upper limits on $\\tan\\beta$ as a function of $m_{A}$ in the hMSSM scenario. The lowest value...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t15","@type":"Dataset","description":"The expected 95% CL upper limits with plus one sigma on $\\tan\\beta$ as a function of $m_{A}$ in the hMSSM...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t16","@type":"Dataset","description":"The expected 95% CL upper limits with minus one sigma on $\\tan\\beta$ as a function of $m_{A}$ in the hMSSM...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t17","@type":"Dataset","description":"The expected 95% CL upper limits with plus two sigma on $\\tan\\beta$ as a function of $m_{A}$ in the hMSSM...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t18","@type":"Dataset","description":"The expected 95% CL upper limits with minus two sigma on $\\tan\\beta$ as a function of $m_{A}$ in the hMSSM...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t19","@type":"Dataset","description":"Acceptance times efficiency for a scalar boson produced by gluon-gluon fusion as a function of the scalar boson mass.","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t20","@type":"Dataset","description":"Acceptance times efficiency for a scalar boson produced by b-associated production as a function of the scalar boson mass.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t21","@type":"Dataset","description":"Observed 95% CL upper limits on the scalar boson production cross section times ditau branching fraction as a function of...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t22","@type":"Dataset","description":"Expected 95% CL upper limits on the scalar boson production cross section times ditau branching fraction as a function of...","name":"Table 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two dimensional likelihood scan of the gluon-gluon fusion cross section times branching fraction, $\\sigma(gg\\phi)\\times B(\\phi\\to\\tau\\tau)$, vs the b-associated production...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t27","@type":"Dataset","description":"Observed two dimensional likelihood scan of the gluon-gluon fusion cross section times branching fraction, $\\sigma(gg\\phi)\\times B(\\phi\\to\\tau\\tau)$, vs the b-associated production...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t28","@type":"Dataset","description":"Observed two dimensional likelihood scan of the gluon-gluon fusion cross section times branching fraction, $\\sigma(gg\\phi)\\times B(\\phi\\to\\tau\\tau)$, vs the b-associated production...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.93071.v4/t29","@type":"Dataset","description":"Observed two dimensional likelihood scan of the gluon-gluon fusion cross section times branching fraction, 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