{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.151813.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2730582"}},{"@id":"https://doi.org/10.1016/j.physletb.2024.138817","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2024","description":"A measurement of the Standard Model Higgs boson produced inassociation with a $W$ or $Z$ boson and decaying into a pair of$\\tau$-leptons is presented.This search is based on proton-proton collision data collected at$\\sqrt{s}=13$\\, TeV by the ATLAS experiment at the LHC correspondingto an integrated luminosity of 140 fb$^{-1}$. For the Higgs bosoncandidate, only final states with at least one $\\tau$-lepton decayinghadronically ($\\tau\\rightarrow \\mathrm{hadrons} + \\nu_\\tau$) areconsidered. For the vector bosons, only leptonic decay channels areconsidered: $Z \\rightarrow \\ell\\ell$ and $W\\rightarrow \\ell\\nu_\\ell$,with $\\ell=e,\\mu$. An excess of events over the expected background is found with anobserved (expected) significance of 4.2 (3.6) standard deviations,providing evidence of the Higgs boson produced in association with avector boson and decaying into a pair of $\\tau$-leptons. The ratio ofthe measured cross-section to the Standard Model prediction is $\\mu_{\\text{VH}}^{\\tau\\tau} = 1.28\\ ^{+0.30}_{-0.29}\\ (\\mathrm{stat.})\\ ^{+0.25}_{-0.21}\\ (\\mathrm{syst.})$.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t1","@type":"Dataset","description":"Distributions of representative kinematic variables in the misidentified background-enriched same-sign region: (a) the Higgs boson transverse momentum (${p_\\text{T}}^H$) in the...","name":"Figure 1a"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t2","@type":"Dataset","description":"Distributions of representative kinematic variables in the misidentified background-enriched same-sign region: (a) the Higgs boson transverse momentum (${p_\\text{T}}^H$) in the...","name":"Figure 1b"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t3","@type":"Dataset","description":"Distributions of representative kinematic variables in the misidentified background-enriched same-sign region: (a) the Higgs boson transverse momentum (${p_\\text{T}}^H$) in the...","name":"Figure 1c"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t4","@type":"Dataset","description":"Distributions of representative kinematic variables in the misidentified background-enriched same-sign region: (a) the Higgs boson transverse momentum ($p_\\text{T}^H$) in the...","name":"Figure 1d"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t5","@type":"Dataset","description":"Post-fit distributions for NN-based analysis of the NN-scores in the $ZH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ (a), $ZH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ (b), $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ (c) and $WH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ (d) categories....","name":"Figure 2a"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t6","@type":"Dataset","description":"Post-fit distributions for NN-based analysis of the NN-scores in the $ZH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ (a), $ZH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ (b), $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ (c) and $WH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ (d) categories....","name":"Figure 2b"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t7","@type":"Dataset","description":"Post-fit distributions for NN-based analysis of the NN-scores in the $ZH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ (a), $ZH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ (b), $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ (c) and $WH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ (d) categories....","name":"Figure 2c"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t8","@type":"Dataset","description":"Post-fit distributions for NN-based analysis of the NN-scores in the $ZH(\\\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ (a), $ZH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ (b), $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ (c) and $WH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ (d) categories....","name":"Figure 2d"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t9","@type":"Dataset","description":"Post-fit yields from the NN-based fit performed with $\\mu_{VH}^{\\tau\\tau}=\\mu_{ZH}^{\\tau\\tau}=\\mu_{WH}^{\\tau\\tau}$. The symbol $-$ is used when no events or $<10^{-2}$ events...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t10","@type":"Dataset","description":"Event yields as a function of $\\log_{10}(S/B)$ for data, background, and a Higgs boson signal with $m_{H} = 125$ GeV....","name":"Figure 3"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t11","@type":"Dataset","description":"The fitted values of the Higgs boson signal strength $\\mu_{VH}^{\\tau\\tau}$ for $m_{H} = 125$ GeV for the $WH$ and $ZH$...","name":"Figure 4"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t12","@type":"Dataset","description":"Post-fit distributions for mass-based analysis for $m_{\\mathrm{MMC}}$ in the (a) $ZH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$, (b) $ZH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$, and for $m_{\\mathrm{2T}}$ in the (c) $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$...","name":"Figure 5a"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t13","@type":"Dataset","description":"Post-fit distributions for mass-based analysis for $m_{\\mathrm{MMC}}$ in the (a) $ZH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$, (b) $ZH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$, and for $m_{\\mathrm{2T}}$ in the (c) $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$...","name":"Figure 5b"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t14","@type":"Dataset","description":"Post-fit distributions for mass-based analysis for $m_{\\mathrm{MMC}}$ in the (a) $ZH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$, (b) $ZH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$, and for $m_{\\mathrm{2T}}$ in the (c) $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$...","name":"Figure 5c"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t15","@type":"Dataset","description":"Post-fit distributions for mass-based analysis for $m_{\\mathrm{MMC}}$ in the (a) $ZH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$, (b) $ZH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$, and for $m_{\\mathrm{2T}}$ in the (c) $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})#...","name":"Figure 5d"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t16","@type":"Dataset","description":"The fitted values from the NN-based fit of the Higgs boson signal strength $\\mu_{VH}^{\\tau\\tau}$ for $m_{H} = 125$ GeV are...","name":"Aux Figure 1 in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t17","@type":"Dataset","description":"Summary table with the expected (exp) and observed (obs) values of the $\\mu^{\\tau\\tau}_{\\text{VH}}$ and the significance resulting from the mass-based...","name":"Aux Table 1 in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t18","@type":"Dataset","description":"Event yields as a function of $\\log_{10}(S/B)$ for data, background, and a Higgs boson signal with $m_{H} = 125$ GeV....","name":"Aux Figure 2 in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t19","@type":"Dataset","description":"Summary table with the expected (exp) and observed (obs) values of the $\\mu^{\\tau\\tau}_{\\text{VH}}$ and the significance resulting from the mass-based...","name":"Aux Table 2 in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t20","@type":"Dataset","description":"The fitted values from the mass-based fit of the Higgs boson signal strength $\\mu_{VH}^{\\tau\\tau}$ for $m_{H} = 125$ GeV are...","name":"Aux Figure 3 in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t21","@type":"Dataset","description":"The fitted values from the mass-based fit of the Higgs boson signal strength $\\mu_{VH}^{\\tau\\tau}$ for $m_{H} = 125$ GeV are...","name":"Aux Figure 4 in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t22","@type":"Dataset","description":"Distributions of $d\\phi({E_{\\mathrm{T}}^{\\mathrm{miss}}},\\tau_{1})$ (left) and $\\eta$ of the leading $p_\\text{T}$ $\\tau_{\\mathrm{had}-\\mathrm{vis}}$ (right) in the $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ $Z\\to\\tau\\tau$ validation region. The hatched...","name":"Aux Figure 5a in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t23","@type":"Dataset","description":"Distributions of $d\\phi({E_{\\mathrm{T}}^{\\mathrm{miss}}},\\tau_{1})$ (left) and $\\eta$ of the leading $p_\\text{T}$ $\\tau_{\\mathrm{had}-\\mathrm{vis}}$ (right) in the $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ $Z\\to\\tau\\tau$ validation region. The hatched...","name":"Aux Figure 5b in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t24","@type":"Dataset","description":"Distributions of the radial distance $dR(\\tau_{1},\\tau_{2})$ between the two $\\tau_{\\mathrm{had}-\\mathrm{vis}}$ (left) and of the ${E_{\\mathrm{T}}^{\\mathrm{miss}}}$ (right) in the $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ $W\\mathrm{...","name":"Aux Figure 6a in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t25","@type":"Dataset","description":"Distributions of the radial distance $dR(\\tau_{1},\\tau_{2})$ between the two $\\tau_{\\mathrm{had}-\\mathrm{vis}}$ (left) and of the ${E_{\\mathrm{T}}^{\\mathrm{miss}}}$ (right) in the $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ $W\\mathrm{...","name":"Aux Figure 6b in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t26","@type":"Dataset","description":"Distributions of the ${m_{\\mathrm{MMC}}}$ (left) and of the $p_\\text{T}$ of the leading $p_\\text{T}$ light lepton (right) in the $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ $t\\bar{t}$...","name":"Aux Figure 7a in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t27","@type":"Dataset","description":"Distributions of the ${m_{\\mathrm{MMC}}}$ (left) and of the $p_\\text{T}$ of the leading $p_\\text{T}$ light lepton (right) in the $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ $t\\bar{t}$...","name":"Aux Figure 7b in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t28","@type":"Dataset","description":"Distributions of the $m_{\\mathrm{2T}}$ (left) and of the $\\eta$ of the leading $p_\\text{T}$ $\\tau_{\\mathrm{had}-\\mathrm{vis}}$ in the $WH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ $Z\\to\\tau\\tau$ validation region....","name":"Aux Figure 8a in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t29","@type":"Dataset","description":"Distributions of the $m_{\\mathrm{2T}}$ (left) and of the $\\eta$ of the leading $p_\\text{T}$ $\\tau_{\\mathrm{had}-\\mathrm{vis}}$ in the $WH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ $Z\\to\\tau\\tau$ validation region....","name":"Aux Figure 8b in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t30","@type":"Dataset","description":"Distributions of the $dR({\\tau_{\\mathrm{lep}}},{\\tau_{\\mathrm{had}}})$ between the two objects associated to the Higgs boson decay and of the invariant mass $m_{\\ell,\\ell}$...","name":"Aux Figure 9a in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t31","@type":"Dataset","description":"Distributions of the $dR({\\tau_{\\mathrm{lep}}},{\\tau_{\\mathrm{had}}})$ between the two objects associated to the Higgs boson decay and of the invariant mass $m_{\\ell,\\ell}$...","name":"Aux Figure 9b in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t32","@type":"Dataset","description":"Distributions of the NN-score in the signal regions sidebands of the $ZH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ (a), $ZH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ (b), $WH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ (c), $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ (d) categories.The...","name":"Aux Figure 10a in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t33","@type":"Dataset","description":"Distributions of the NN-score in the signal regions sidebands of the $ZH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ (a), $ZH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ (b), $WH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ (c), $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ (d) categories.The...","name":"Aux Figure 10b in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t34","@type":"Dataset","description":"Distributions of the NN-score in the signal regions sidebands of the $ZH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ (a), $ZH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ (b), $WH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ (c), $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ (d) categories.The...","name":"Aux Figure 10c in paper"},{"@id":"https://doi.org/10.17182/hepdata.151813.v1/t35","@type":"Dataset","description":"Distributions of the NN-score in the signal regions sidebands of the $ZH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ (a), $ZH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ (b), $WH(\\tau_{\\mathrm{lep}}\\tau_{\\mathrm{had}})$ (c), $WH(\\tau_{\\mathrm{had}}\\tau_{\\mathrm{had}})$ (d) categories.The...","name":"Aux Figure 10d in paper"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2730582?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/151813"}],"inLanguage":"en","name":"Evidence for the $VH, H\\rightarrow \\tau\\tau$ process with the ATLAS detector in Run 2","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2730582?version=1","version":1}