{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.132012.v1/t2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2027827"}},{"@id":"https://doi.org/10.1140/epjc/s10052-022-10472-0","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2022","description":"Comparison of single-ratio two-particle correlation functions, C2data(Q) and C2MC(Q), with the two-particle double-ratio correlation function, R2(Q), for the high-multiplicity track...","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1348549/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1348549/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1348549/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1348549/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1348549/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2027827?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/132012"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.132012.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins2027827?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.132012.v1","@type":"Dataset","description":"Two-particle Bose-Einstein correlations in pp collisions at \u221as=13 TeV measured with the ATLAS detector at the LHC.\n\nThis paper presents studies  of Bose-Einstein correlations (BEC) in  proton-proton  collisions at  a centre-of-mass energy of  13 TeV, using data from the ATLAS detector at the CERN Large Hadron Collider.  Data were collected in a special low-luminosity configuration with a minimum-bias trigger and a  high-multiplicity track trigger,  accumulating integrated luminosities of 151 $\\mu$b$^{-1}$   and 8.4 nb$^{-1}$  respectively.  The BEC are measured for pairs of like-sign charged particles,  each with $|\\eta|$ &lt; 2.5, for two kinematic ranges: the first with particle $p_T$ &gt; 100 MeV  and the second with particle $p_T$ &gt; 500 MeV. The BEC parameters, characterizing  the   source radius and particle correlation strength, are investigated as functions of charged-particle multiplicity (up to 300) and average transverse momentum of the pair (up to 1.5 GeV). The double-differential  dependence on charged-particle multiplicity and average transverse momentum  of the pair is also studied. The BEC radius is found to be independent of the charged-particle multiplicity  for high charged-particle multiplicity (above 100), confirming a previous observation at lower energy.  This saturation occurs independent of the transverse momentum of the pair.","name":"Two-particle Bose-Einstein correlations in pp collisions at ${\\sqrt{s} = 13}$ TeV measured with the ATLAS detector at the LHC","url":"https://www.hepdata.net/record/ins2027827?version=1"},"keywords":"P P --> CHARGED X, C2, R2, Inclusive, Integrated Cross Section, Cross Section, Proton-Proton Scattering, 13000.0","name":"Figure 1b","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/135076","version":1}
