{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.77761.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1512305"}},{"@id":"https://doi.org/10.1038/nphys4208","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2017","description":"CERN-LHC.  Measurement of the total fiducial cross section for light-by-light scattering in lead-lead collisions at a centre-of-mass energy of 5.02 TeV with 0.48 nb^-1 of data collected in 2015.  The final states used are 2 photons and no further activity in the detector.\n\nThe fiducial region is defined as:\n- 2Gamma\n- pt_Gamma > 3 GeV\n- |eta_Gamma| < 2.4\n- m_GammaGamma must be above 6 GeV\n- pt_GammaGamma must be below 2 GeV\n- aco_GammaGamma must be below 0.01","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.77761.v1/t3","@type":"Dataset","description":"Detector-level diphoton acoplanarity distribution","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.77761.v1/t2","@type":"Dataset","description":"Detector-level diphoton invariant mass distribution","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.77761.v1/t3","@type":"Dataset","description":"The measured total fiducial cross section","name":"Table 3"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1512305?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/77761"}],"inLanguage":"en","name":"Evidence for light-by-light scattering in heavy-ion collisions with the ATLAS detector at the LHC","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1512305?version=1","version":1}