{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.132012.v1","@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":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2022","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 $|\\eta|$ < 2.5, for two kinematic ranges: the first with particle $p_T$ > 100 MeV  and the second with particle $p_T$ > 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.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.132012.v1/t1","@type":"Dataset","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...","name":"Figure 1a"},{"@id":"https://doi.org/10.17182/hepdata.132012.v1/t2","@type":"Dataset","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...","name":"Figure 1b"},{"@id":"https://doi.org/10.17182/hepdata.132012.v1/t3","@type":"Dataset","description":"The Bose-Einstein correlation (BEC) parameter R as a function of nch for MB events using different MC generators in the...","name":"Figure 2a"},{"@id":"https://doi.org/10.17182/hepdata.132012.v1/t4","@type":"Dataset","description":"The Bose-Einstein correlation (BEC) parameter R as a function of nch for HMT events using different MC generators in the...","name":"Figure 2b"},{"@id":"https://doi.org/10.17182/hepdata.132012.v1/t5","@type":"Dataset","description":"The Bose-Einstein correlation (BEC) parameter R as a function of kT for MB events using different MC generators in the...","name":"Figure 2c"},{"@id":"https://doi.org/10.17182/hepdata.132012.v1/t6","@type":"Dataset","description":"The Bose-Einstein correlation (BEC) parameter λ as a function of kT for MB events using different MC generators in the...","name":"Figure 2d"},{"@id":"https://doi.org/10.17182/hepdata.132012.v1/t7","@type":"Dataset","description":"The two-particle double-ratio correlation function, R2(Q), for pp collisions for track pT >100 MeV at √s=13 TeV in the multiplicity interval 71...","name":"Figure 3a"},{"@id":"https://doi.org/10.17182/hepdata.132012.v1/t8","@type":"Dataset","description":"The two-particle double-ratio correlation function, R2(Q), for pp collisions for track pT >100 MeV at √s=13 TeV in the multiplicity interval 231...","name":"Figure 3b"},{"@id":"https://doi.org/10.17182/hepdata.132012.v1/t9","@type":"Dataset","description":"The dependence of the correlation strength, λ(mch), on rescaled multiplicity, mch, obtained from the exponential fit of the R2(Q) correlation...","name":"Figure 4a (MB 100MeV)"},{"@id":"https://doi.org/10.17182/hepdata.132012.v1/t10","@type":"Dataset","description":"The dependence of the correlation strength, λ(mch), on rescaled multiplicity, mch, obtained from the exponential fit of the R2(Q) correlation...","name":"Figure 4a (HMT 100MeV)"},{"@id":"https://doi.org/10.17182/hepdata.132012.v1/t11","@type":"Dataset","description":"The dependence of the correlation strength, λ(mch), on rescaled multiplicity, mch, obtained from the exponential fit of the R2(Q) correlation...","name":"Figure 4a (MB 500MeV)"},{"@id":"https://doi.org/10.17182/hepdata.132012.v1/t12","@type":"Dataset","description":"The dependence of the correlation strength, λ(mch), on rescaled multiplicity, mch, obtained from the exponential fit of the R2(Q) correlation...","name":"Figure 4a (HMT 500MeV)"},{"@id":"https://doi.org/10.17182/hepdata.132012.v1/t13","@type":"Dataset","description":"The dependence of the source radius, R(mch), on mch. 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