{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.87256.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1723858"}},{"@id":"https://doi.org/10.1016/j.physletb.2019.07.031","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2019","description":"The inclusive production rates of isolated, prompt photons in $p$+Pb collisions at $\\sqrt{s_{NN}}=8.16$ TeV are studied with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb^\u22121 recorded in 2016. The cross-section and nuclear modification factor R_{pPb} are measured as a function of photon transverse energy from 20 GeV to 550 GeV and in three nucleon-nucleon centre-of-mass pseudorapidity regions, (\u22122.83,\u22122.02), (\u22121.84,0.91), and (1.09,1.90).","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.87256.v1/t1","@type":"Dataset","description":"The measured cross sections for prompt, isolated photons with rapidity in (1.09,1.90).","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.87256.v1/t2","@type":"Dataset","description":"The measured cross sections for prompt, isolated photons with rapidity in (\u22121.84,0.91).","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.87256.v1/t3","@type":"Dataset","description":"The measured cross sections for prompt, isolated photons with rapidity in (\u22122.83,\u22122.02).","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.87256.v1/t4","@type":"Dataset","description":"The nuclear modification factor R_pPb for prompt, isolated photons with rapidity in (1.09,1.90).","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.87256.v1/t5","@type":"Dataset","description":"The nuclear modification factor R_pPb for prompt, isolated photons with rapidity in (\u22121.84,0.91).","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.87256.v1/t6","@type":"Dataset","description":"The nuclear modification factor R_pPb for prompt, isolated photons with rapidity in (\u22122.83,\u22122.02).","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.87256.v1/t7","@type":"Dataset","description":"The ratio of R_{pPb} from rapidity (1.09,1.90) to that of rapidity (\u22122.83,\u22122.02).","name":"Table 7"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1723858?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/87256"}],"inLanguage":"en","name":"Measurement of prompt photon production in $\\sqrt{s_\\mathrm{NN}} = 8.16$ TeV $p$+Pb collisions with ATLAS","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1723858?version=1","version":1}