{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.88276.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1716441"}},{"@id":"https://doi.org/10.1103/PhysRevC.100.044902","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2022","description":"Azimuthal correlations of charged particles in xenon-xenon  collisions at a center-of-mass energy per nucleon pair of $ \\sqrt{s_{_\\mathrm{NN}}} =  5.44~$TeV are studied. The data were collected by the CMS experiment at the LHC with a total integrated luminosity of $3.42~\\mathrm{\\mu b}^{-1}$.  The collective motion of the system formed in the collision is parameterized by a Fourier expansion of the azimuthal particle density distribution. The azimuthal anisotropy coefficients $v_{2}$, $v_{3}$, and $v_{4}$ are obtained by the scalar-product, two-particle correlation, and  multiparticle correlation methods. Within a hydrodynamic picture, these methods have different sensitivities to  non-collective and fluctuation effects. The dependence of the Fourier coefficients on the size of the colliding system is explored by comparing the xenon-xenon results with equivalent lead-lead data. Model calculations that include initial-state fluctuation effects are also compared to the experimental results. The observed angular correlations provide new constraints on the hydrodynamic description of heavy ion collisions.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t1","@type":"Dataset","description":"Elliptic-flow coefficients $v_2$ based on the two-particle correlations technique, as functions of transverse momentum and in bins of centrality. The...","name":"Figure 1a"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t2","@type":"Dataset","description":"Elliptic-flow coefficients $v_2$ based on the scalar-product technique, as functions of transverse momentum and in bins of centrality. The results...","name":"Figure 1b"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t3","@type":"Dataset","description":"Elliptic-flow coefficients $v_2$ based on the four-particle correlations technique, as functions of transverse momentum and in bins of centrality. The...","name":"Figure 1c"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t4","@type":"Dataset","description":"Elliptic-flow coefficients $v_2$ based on the six-particle correlations technique, as functions of transverse momentum and in bins of centrality. The...","name":"Figure 1d"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t5","@type":"Dataset","description":"Elliptic-flow coefficients $v_2$ based on the eight-particle correlations technique, as functions of transverse momentum and in bins of centrality. The...","name":"Figure 1e"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t6","@type":"Dataset","description":"Triangular-flow coefficients $v_3$ based on the two-particle correlations technique, as functions of transverse momentum and in bins of centrality. The...","name":"Figure 2a"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t7","@type":"Dataset","description":"Triangular-flow coefficients $v_3$ based on the scalar-product technique, as functions of transverse momentum and in bins of centrality. The results...","name":"Figure 2b"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t8","@type":"Dataset","description":"Triangular-flow coefficients $v_3$ based on the four-particle correlations technique, as functions of transverse momentum and in bins of centrality. The...","name":"Figure 2c"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t9","@type":"Dataset","description":"The $v_4$ coefficients based on the two-particle correlations technique, as functions of transverse momentum and in bins of centrality. The...","name":"Figure 3a"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t10","@type":"Dataset","description":"The $v_4$ coefficients based on the scalar-product technique, as functions of transverse momentum and in bins of centrality. The results...","name":"Figure 3b"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t11","@type":"Dataset","description":"Centrality dependence of the spectrum-weighted $v_2$ flow harmonics with $0.3 < p_{\\mathrm{T}} < 3.0~\\mathrm{GeV}/c$. The $v_2$ results are shown for...","name":"Figure 4a"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t12","@type":"Dataset","description":"Centrality dependence of the spectrum-weighted $v_3$ flow harmonics with $0.3 < p_{\\mathrm{T}} < 3.0~\\mathrm{GeV}/c$. The results are shown for two-...","name":"Figure 4b"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t13","@type":"Dataset","description":"Centrality dependence of the spectrum-weighted $v_4$ flow harmonics with $0.3 < p_{\\mathrm{T}} < 3.0~\\mathrm{GeV}/c$. The results are shown for two-particle...","name":"Figure 4c"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t14","@type":"Dataset","description":"Centrality dependence of $v_2\\{4\\}/v_2\\{2\\}$ ratios.","name":"Figure 5a"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t15","@type":"Dataset","description":"Centrality dependence of $v_2\\{6\\}/v_2\\{4\\}$ ratios.","name":"Figure 5b"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t16","@type":"Dataset","description":"Centrality dependence of $v_3\\{4\\}/v_3\\{2\\}$ ratios.","name":"Figure 5c"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t17","@type":"Dataset","description":"The $v_2$ results measured with two-particle correlations from PbPb collisions at $5.02~$TeV, shown as a function of $p_{\\mathrm{T}}$ in eleven...","name":"Figure 6"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t18","@type":"Dataset","description":"The $v_3$ results measured with two-particle correlations from PbPb collisions at $5.02~$TeV, shown as a function of $p_{\\mathrm{T}}$ in eleven...","name":"Figure 7"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t19","@type":"Dataset","description":"The $v_4$ results measured with two-particle correlations from PbPb collisions at $5.02~$TeV, shown as a function of $p_{\\mathrm{T}}$ in eleven...","name":"Figure 8"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t20","@type":"Dataset","description":"Ratios of the $v_2$ harmonic coefficients from two-particle correlations in XeXe and PbPb collisions as functions of $p_{\\mathrm{T}}$ in 11...","name":"Figure 9a"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t21","@type":"Dataset","description":"Ratios of the $v_3$ harmonic coefficients from two-particle correlations in XeXe and PbPb collisions as functions of $p_{\\mathrm{T}}$ in 11...","name":"Figure 9b"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t22","@type":"Dataset","description":"Ratios of the $v_4$ harmonic coefficients from two-particle correlations in XeXe and PbPb collisions as functions of $p_{\\mathrm{T}}$ in 11...","name":"Figure 9c"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t23","@type":"Dataset","description":"Centrality dependence of the spectrum-weighted $v_2$, $v_3$, and $v_4$ harmonic coefficients from two-particle correlations method for $0.3 < p_{\\mathrm{T}} <...","name":"Figure 10a"},{"@id":"https://doi.org/10.17182/hepdata.88276.v1/t24","@type":"Dataset","description":"Ratios of the $v_2$, $v_3$, and $v_4$ harmonic coefficients from two-particle correlations in XeXe and PbPb collisions as functions or...","name":"Figure 10b"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1716441?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/88276"}],"inLanguage":"en","name":"Charged-particle angular correlations in XeXe collisions at $\\sqrt{s_{_\\mathrm{NN}}}=$ 5.44 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1716441?version=1","version":1}