{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.136027.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2653725"}},{"@id":"https://doi.org/10.1007/JHEP07(2023)125","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2024","description":"CERN-ATLAS. Search for high-mass $W\\gamma$ and $Z\\gamma$ resonances using hadronic $W/Z$ boson decays from 139 fb$^{-1}$ of $pp$ collisions at $\\sqrt{s}=$ 13 TeV with the ATLAS detector\n\nA search for high-mass charged and neutral bosons decaying to $W\\gamma$  and $Z\\gamma$ final states is presented in this paper. The analysis uses a data sample of $\\sqrt{s} = 13$~TeV proton--proton collisions with an integrated luminosity of 139~fb$^{-1}$ collected by the ATLAS detector during LHC Run~2 operation. The sensitivity of the search is determined using models of the production and decay of spin-1 charged bosons and spin-0/2 neutral bosons. The range of resonance masses explored extends from 1.0~TeV to 6.8~TeV. At these high resonance masses, it is beneficial to target the hadronic decays of the $W$ and $Z$ bosons because of their large branching fractions. The decay products of the high-momentum $W/Z$ bosons are strongly collimated and boosted-boson tagging techniques are employed to improve the sensitivity. No evidence of a signal above the Standard Model backgrounds is observed, and upper limits on the production cross-sections of these bosons times their branching fractions to $W\\gamma$ and $Z\\gamma$ are derived for various boson production models.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t1","@type":"Dataset","description":"The jet mass distribution of large-$R$ jets originating from the hadronic decay of $W$ and $Z$ bosons produced from the...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t2","@type":"Dataset","description":"The jet mass distribution of large-$R$ jets originating from the hadronic decay of $W$ and $Z$ bosons produced from the...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t3","@type":"Dataset","description":"Total efficiencies for the selection of signal events after categorization and application of the tighter photon $E_{\\mathrm{T}}^{\\gamma}$ selection used to...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t4","@type":"Dataset","description":"Total efficiencies for the selection of signal events after categorization and application of the tighter photon $E_{\\mathrm{T}}^{\\gamma}$ selection used to...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t5","@type":"Dataset","description":"Total efficiencies for the selection of signal events after categorization and application of the tighter photon $E_{\\mathrm{T}}^{\\gamma}$ selection used to...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t6","@type":"Dataset","description":"Total efficiencies for the selection of signal events after categorization and application of the tighter photon $E_{\\mathrm{T}}^{\\gamma}$ selection used to...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t7","@type":"Dataset","description":"The $m_{J\\gamma}$ distributions of data events selected for the spin-1 $q\\bar{q'}\\to X^{\\pm} \\to W^{\\pm}\\gamma$ search in the D2 category. The...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t8","@type":"Dataset","description":"The $m_{J\\gamma}$ distributions of data events selected for the spin-1 $q\\bar{q'}\\to X^{\\pm} \\to W^{\\pm}\\gamma$ search in the WMASS category. The...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t9","@type":"Dataset","description":"The $m_{J\\gamma}$ distributions of data events selected for the spin-0 $gg \\to X^{0} \\to Z\\gamma$ search in the BTAG category....","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t10","@type":"Dataset","description":"The $m_{J\\gamma}$ distributions of data events selected for the spin-0 $gg \\to X^{0} \\to Z\\gamma$ search in the D2 category....","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t11","@type":"Dataset","description":"The $m_{J\\gamma}$ distributions of data events selected for the spin-0 $gg \\to X^{0} \\to Z\\gamma$ search in the ZMASS category....","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t12","@type":"Dataset","description":"The $m_{J\\gamma}$ distributions of data events selected for the spin-2 $gg \\to X^{0} \\to Z\\gamma$ search in the BTAG category....","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t13","@type":"Dataset","description":"The $m_{J\\gamma}$ distributions of data events selected for the spin-2 $gg \\to X^{0} \\to Z\\gamma$ search in the D2 category....","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t14","@type":"Dataset","description":"The $m_{J\\gamma}$ distributions of data events selected for the spin-2 $gg \\to X^{0} \\to Z\\gamma$ search in the ZMASS category....","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t15","@type":"Dataset","description":"The $m_{J\\gamma}$ distributions of data events selected for the spin-2 $q\\bar{q} \\to X^{0} \\to Z\\gamma$ search in the BTAG category....","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t16","@type":"Dataset","description":"The $m_{J\\gamma}$ distributions of data events selected for the spin-2 $q\\bar{q} \\to X^{0} \\to Z\\gamma$ search in the D2 category....","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t17","@type":"Dataset","description":"The $m_{J\\gamma}$ distributions of data events selected for the spin-2 $q\\bar{q} \\to X^{0} \\to Z\\gamma$ search in the ZMASS category....","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t18","@type":"Dataset","description":"The 95% CL upper limits on $\\sigma(pp\\to X)\\times B(X\\to W/Z\\gamma)$ as a function of $m_{X}$ for spin-0 $gg \\to X^{0}...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t19","@type":"Dataset","description":"The 95% CL upper limits on $\\sigma(pp\\to X)\\times B(X\\to W/Z\\gamma)$ as a function of $m_{X}$ for spin-2 $gg \\to X^{0}...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t20","@type":"Dataset","description":"The 95% CL upper limits on $\\sigma(pp\\to X)\\times B(X\\to W/Z\\gamma)$ as a function of $m_{X}$ for spin-2 $q\\bar{q} \\to X^{0}...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t21","@type":"Dataset","description":"The 95% CL upper limits on $\\sigma(pp\\to X)\\times B(X\\to W/Z\\gamma)$ as a function of $m_{X}$ for spin-1 $q\\bar{q'}\\to X^{\\pm} \\to...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t22","@type":"Dataset","description":"The jet mass distribution of large-$R$ jets originating from the hadronic decay of $W$ and $Z$ bosons produced from the...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t23","@type":"Dataset","description":"The photon $E_{T}$ selection criteria as a function of resonance mass for D2 categories. Selections for four different signal channels...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.136027.v1/t24","@type":"Dataset","description":"The photon $E_{T}$ selection criteria as a function of resonance mass for ZMASS or WMASS categories. Selections for four different...","name":"Table 24"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2653725?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/136027"}],"inLanguage":"en","name":"Search for high-mass $W\\gamma$ and $Z\\gamma$ resonances using hadronic W/Z boson decays from 139 fb$^{-1}$ of $pp$ collisions at $\\sqrt{s}=$ 13 TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2653725?version=1","version":1}