{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.86566.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1518782"}},{"@id":"https://doi.org/10.1016/j.physletb.2017.12.050","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"LHCf Collaboration"},"creator":{"@type":"Organization","name":"LHCf Collaboration"},"datePublished":"2019","description":"Inclusive differential production cross section of forward photons produced in p-p collisions at $\\mathrm{\\sqrt{s}=13\\,TeV}$. Cross section is expressed as a function of energy in two different pseudorapidity regions, namely $\\eta>10.94$ and $8.81<\\eta<8.99$. The measurements refer to all photons directly produced in the collisions or resulting from the decay of short life particles ($\\mathrm{c \\tau<1\\,cm}$).","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.86566.v1/t1","@type":"Dataset","description":"Inclusive photon production cross section in $\\eta > 10.94$","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.86566.v1/t2","@type":"Dataset","description":"Inclusive photon production cross section in $8.81<\\eta<8.99$","name":"Table 2"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1518782?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/86566"}],"inLanguage":"en","name":"Measurement of forward photon production cross-section in proton\u2013proton collisions at $\\sqrt{s}$ = 13 TeV with the LHCf detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1518782?version=1","version":1}