{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.85763.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1717700"}},{"@id":"https://doi.org/10.1016/j.physletb.2019.03.067","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2019","description":"CERN-LHC. Search for localized excesses in dijet mass distributions of low-dijet-mass events produced in association with a high transverse energy photon.\n\nTwo variants are presented, one which makes no jet flavour requirements and one which requires both jets to be tagged as b-jets. The observed mass distributions are consistent with multi-jet processes in the Standard Model. The data are used to set upper limits on the production cross-section for a benchmark $Z'$ model and, separately, on generic Gaussian-shaped contributions to the distributions, extending the current ATLAS constraints on dijet resonances to the mass range between 200 and 350 GeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.85763.v1/t1","@type":"Dataset","description":"Dijet mass distribution for the flavour inclusive category. Data, estimated background and uncertainties are shown. Events are collected using the...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.85763.v1/t2","@type":"Dataset","description":"Dijet mass distribution for the flavour inclusive category. Data, estimated background and uncertainties are shown. Events are collected using the...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.85763.v1/t3","@type":"Dataset","description":"Dijet mass distribution for the b-tagged category. Data, estimated background and uncertainties are shown. Events are collected using the single-photon...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.85763.v1/t4","@type":"Dataset","description":"Dijet mass distribution for the b-tagged category. Data, estimated background and uncertainties are shown. Events are collected using the combined...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.85763.v1/t5","@type":"Dataset","description":"Upper limits on Gaussian-shape contributions to the dijet mass distributions from the flavour-inclusive category and masses below 450 GeV, for...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.85763.v1/t6","@type":"Dataset","description":"Upper limits on Gaussian-shape contributions to the dijet mass distributions from the flavour-inclusive category and masses above 450 GeV, for...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.85763.v1/t7","@type":"Dataset","description":"Upper limits on Gaussian-shape contributions to the dijet mass distributions from the b-tagged category and masses below 450 GeV, for...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.85763.v1/t8","@type":"Dataset","description":"Upper limits on Gaussian-shape contributions to the dijet mass distributions from the b-tagged category and masses above 450 GeV, for...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.85763.v1/t9","@type":"Dataset","description":"Kinematic acceptance values predicted for the $Z'$ model as a function of mass $m_{Z'}$ for the flavour-inclusive category using the...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.85763.v1/t10","@type":"Dataset","description":"Kinematic acceptance values predicted for the $Z'$ model as a function of mass $m_{Z'}$ for the flavour-inclusive category using the...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.85763.v1/t11","@type":"Dataset","description":"Kinematic acceptance values predicted for the $Z'$ model as a function of mass $m_{Z'}$ for the b-tagged category using the...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.85763.v1/t12","@type":"Dataset","description":"Kinematic acceptance values predicted for the $Z'$ model as a function of mass $m_{Z'}$ for the b-tagged category using the...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.85763.v1/t13","@type":"Dataset","description":"Reconstruction efficiency for $Z'$ model, flavour inclusive category, single-photon trigger.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.85763.v1/t14","@type":"Dataset","description":"Reconstruction efficiency for $Z'$ model, flavour inclusive category, combined trigger.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.85763.v1/t15","@type":"Dataset","description":"Reconstruction efficiency for $Z'$ model, b-tagged category, single-photon trigger.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.85763.v1/t16","@type":"Dataset","description":"Reconstruction efficiency for $Z'$ model, b-tagged category, combined trigger.","name":"Table 16"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1717700?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/85763"}],"inLanguage":"en","name":"Search for low-mass resonances decaying into two jets and produced in association with a photon using $pp$ 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/ins1717700?version=1","version":1}