{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.79924.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1609773"}},{"@id":"https://doi.org/10.1016/j.physletb.2017.10.039","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2017","description":"CERN-LHC. Search for new phenomena in high-mass diphoton final states using 37 fb^\u22121 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector in 2015 and 2016. The final states used are 2 photons.\n\nThe fiducial region for the spin-0 resonance search is defined as:\n- 2 photons\n- E_T > 0.4 m_gamgam for the photon with leading E_T, and E_T > 0.3 m_gamgam for the photon with sub-leading E_T\n- |eta_gam| < 2.37\n- An isolation requirement using all particles with lifetime greater than 10 ps at the generator level in a cone of Delta_R = 0.4 around the photon direction: E^iso_T< 0.05 E_T+ 6 GeV.\n\nFor the spin-2 resonance search, the acceptance and efficiencies are assumed to be those obtained from MC simulation of KK graviton decays.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.79924.v1/t1","@type":"Dataset","description":"Upper limits on the fiducial cross section times branching ratio to two photons at centre-of-mass energy of 13 TeV of...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.79924.v1/t2","@type":"Dataset","description":"Upper limits on the fiducial cross section times branching ratio to two photons at centre-of-mass energy of 13 TeV of...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.79924.v1/t3","@type":"Dataset","description":"Upper limits on the fiducial cross section times branching ratio to two photons at centre-of-mass energy of 13 TeV of...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.79924.v1/t4","@type":"Dataset","description":"Upper limits on the fiducial cross section times branching ratio to two photons at centre-of-mass energy of 13 TeV of...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.79924.v1/t5","@type":"Dataset","description":"Upper limits on the production cross section times branching ratio to two photons at centre-of-mass energy of 13 TeV of...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.79924.v1/t6","@type":"Dataset","description":"Upper limits on the production cross section times branching ratio to two photons at centre-of-mass energy of 13 TeV of...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.79924.v1/t7","@type":"Dataset","description":"Upper limits on the production cross section times branching ratio to two photons at centre-of-mass energy of 13 TeV of...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.79924.v1/t8","@type":"Dataset","description":"Upper limits on the production cross section times branching ratio to two photons at centre-of-mass energy of 13 TeV of...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.79924.v1/t9","@type":"Dataset","description":"Distribution of the diphoton invariant mass for data events passing the spin-0 selection. The data points are plotted at the...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.79924.v1/t10","@type":"Dataset","description":"Distribution of the diphoton invariant mass for data events passing the spin-2 selection. The data points are plotted at the...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.79924.v1/t11","@type":"Dataset","description":"Fiducial acceptance and product of the fiducial acceptance times the combined reconstruction and identification efficiency as a function of the...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.79924.v1/t12","@type":"Dataset","description":"Fiducial acceptance and product of the fiducial acceptance times the combined reconstruction and identification efficiency as a function of the...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.79924.v1/t13","@type":"Dataset","description":"Fiducial acceptance and product of the fiducial acceptance times the combined reconstruction and identification efficiency as a function of the...","name":"Table 13"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1609773?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/79924"}],"inLanguage":"en","name":"Search for new phenomena in high-mass diphoton final states using 37 fb$^{-1}$ of proton--proton collisions collected 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/ins1609773?version=1","version":1}