{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.131600.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2178061"}},{"@id":"https://doi.org/10.1007/JHEP07(2023)155","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2023","description":"CERN-LHC. Search for boosted resonances in the 10 to 70 GeV mass range and decaying into two photons using 138 $fb^{-1}$ of 13 TeV pp collision data with the ATLAS detector. \n\nThe fiducial region for this resonance search is defined as:\n- 2 photons\n- $p^{\\gamma\\gamma}_T$ > 50 GeV\n- $|\\eta^{\\gamma}|$ < 2.37\n- An isolation requirement using all particles with lifetime greater than 10 ps at the generator level in a cone of $\\Delta R$ = 0.2 around the photon direction: $E^{iso}_{T}< 0.065 E_{T}$.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.131600.v1/t1","@type":"Dataset","description":"The expected and observed upper limits at 95\\% CL on the fiducial cross-section times branching ratio to two photons of...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.131600.v1/t2","@type":"Dataset","description":"Diphoton invariant mass in the signal region using a 0.1 GeV binning.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.131600.v1/t3","@type":"Dataset","description":"Parametrization of the $C_{X}$ factor, defined as the ratio between the number of reconstructed signal events passing the analysis cuts...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.131600.v1/t4","@type":"Dataset","description":"Parametrization of the $A_{X}$ factor, defined as the fraction of diphoton resonances satisfying the fiducial acceptance at the particle level,...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.131600.v1/t5","@type":"Dataset","description":"The correction factor, $C_{X}$, defined as the ratio between the number of reconstructed signal events passing the analysis cuts and...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.131600.v1/t6","@type":"Dataset","description":"Effect of event selections on a scalar MC signal sample generated for $m_{X}$ = 15 GeV and on the data....","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.131600.v1/t7","@type":"Dataset","description":"Parameterization of the Double Sided Crystal Ball function parameters describing the scalar mass resolution model as a function of $m_{X}$...","name":"Table 7"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2178061?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/131600"}],"inLanguage":"en","name":"Search for boosted diphoton resonances in the 10 to 70 GeV mass range using 138 fb$^{-1}$ of 13 TeV $pp$ collisions with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2178061?version=1","version":1}