{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.82605.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1672010"}},{"@id":"https://doi.org/10.1103/PhysRevD.98.032015","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"CERN-ATLAS. Search for heavy resonances decaying to a photon and a hadronically decaying Z/W/H boson in pp collisions at sqrt{s} = 13 TeV with the ATLAS detector.\n\nMany extensions of the Standard Model predict new resonances decaying to a Z, W, or Higgs boson and a photon. This paper presents a search for such resonances produced in pp collision at sqrt{s}=13 TeV using a dataset with an integrated luminosity of 36.1/fb collected by the ATLAS detector at the Large Hadron Collider. The Z/W/H bosons are identified through their decays to hadrons. The data are found to be consistent with the Standard Model expectation in the entire investigated mass range. Upper limits are set on the production cross section times branching fraction for resonance decays to Z/W+gamma in the mass range from 1.0 to 6.8 TeV, and for the first time into H+gamma in the mass range from 1.0 to 3.0 TeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t1","@type":"Dataset","description":"Efficiencies for gg->X(J=0)->Zgamma signal events to pass the category selections as a function of the resonance mass.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t2","@type":"Dataset","description":"Efficiencies for qqbar->X(J=2)->Zgamma signal events to pass the category selections as a function of the resonance mass.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t3","@type":"Dataset","description":"Efficiencies for gg->X(J=2)->Zgamma signal events to pass the category selections as a function of the resonance mass.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t4","@type":"Dataset","description":"Efficiencies for qqbar->X(J=1)->Wgamma signal events to pass the category selections as a function of the resonance mass.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t5","@type":"Dataset","description":"Efficiencies for qqbar->X(J=1)->Hgamma signal events to pass the category selections as a function of the resonance mass.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t6","@type":"Dataset","description":"Distribution of the reconstructed J+gamma invariant mass in Z+gamma search BTAG category.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t7","@type":"Dataset","description":"Distribution of the reconstructed J+gamma invariant mass in Z+gamma search D2 category.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t8","@type":"Dataset","description":"Distribution of the reconstructed J+gamma invariant mass in Z+gamma search VMASS category.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t9","@type":"Dataset","description":"Distribution of the reconstructed J+gamma invariant mass in Z+gamma search ELSE category.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t10","@type":"Dataset","description":"Distribution of the reconstructed J+gamma invariant mass in W+gamma search D2 category.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t11","@type":"Dataset","description":"Distribution of the reconstructed J+gamma invariant mass in W+gamma search VMASS category.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t12","@type":"Dataset","description":"Distribution of the reconstructed J+gamma invariant mass in W+gamma search ELSE category.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t13","@type":"Dataset","description":"Distribution of the reconstructed J+gamma invariant mass in H+gamma search BTAG category.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t14","@type":"Dataset","description":"The 95% CL upper limits on cross section times branching ratio for spin-0 resonance decaying to Zgamma.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t15","@type":"Dataset","description":"The 95% CL upper limits on cross section times branching ratio for gluon-gluon fusion production spin-2 resonance decaying to Zgamma.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t16","@type":"Dataset","description":"The 95% CL upper limits on cross section times branching ratio for quark-antiquark annihilation production spin-2 resonance decaying to Zgamma.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t17","@type":"Dataset","description":"The 95% CL upper limits on cross section times branching ratio for spin-1 resonance decaying to Wgamma.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.82605.v1/t18","@type":"Dataset","description":"The 95% CL upper limits on cross section times branching ratio for spin-1 resonance decaying to Hgamma.","name":"Table 18"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1672010?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/82605"}],"inLanguage":"en","name":"Search for heavy resonances decaying to a photon and a hadronically decaying $Z/W/H$ boson in $pp$ collisions at $\\sqrt{s}=13$ $\\mathrm{TeV}$ with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1672010?version=1","version":1}