{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.85727.v3","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1672790"}},{"@id":"https://doi.org/10.1016/j.physletb.2018.10.052","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2024","description":"Transverse momentum $(p_{\\rm T})$ spectra of charged particles was measured at mid-pseudorapidity in Xe\u2013Xe collisions at $\\sqrt{s_{\\rm NN}} = 5.44$ TeV, in the kinematic range of $0.15<p_{\\rm T}<50$ GeV/c and $|\\eta|<0.8$. The pp reference at $\\sqrt{s} = 5.44$ TeV is interpolated between existing pp measurements at $\\sqrt{s} = 5.02$ and $7$ TeV. The nuclear modification factor is calculated for Xe-Xe and Pb-Pb collisions at similar center-of-mass energy, as a function of $p_{\\rm T}$ and the charged particle multiplicity density. The average transverse momentum $\\langle p_{\\rm T} \\rangle$ is calculated for both systems, as well as the ratio between them.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.85727.v3/t1","@type":"Dataset","description":"Transverse momentum spectra of charged particles in XeXe collisions in nine centrality classes.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.85727.v3/t2","@type":"Dataset","description":"Interpolated pp reference spectrum and invariant cross section.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.85727.v3/t3","@type":"Dataset","description":"Nuclear modification factor for XeXe. Additional systematic error: 0-5 pct data: +6.1 pct -6.1 pct 5-10 pct data: +6.6 pct...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.85727.v3/t4","@type":"Dataset","description":"Ratio of transverse momentum spectra in Xe-Xe and Pb-Pb.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.85727.v3/t5","@type":"Dataset","description":"Raa vs $\\langle dNch/d\\eta \\rangle$.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.85727.v3/t6","@type":"Dataset","description":"Raa vs $\\langle dNch/d\\eta \\rangle$.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.85727.v3/t7","@type":"Dataset","description":"Raa vs $\\langle dNch/d\\eta \\rangle$.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.85727.v3/t8","@type":"Dataset","description":"Average transverse momentum vs centrality percentage for PbPb and XeXe. And the ratio between collision systems.","name":"Table 8"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1672790?version=3"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/85727"}],"inLanguage":"en","name":"Transverse momentum spectra and nuclear modification factors of charged particles in Xe-Xe collisions at $\\sqrt{s_{\\rm NN}}$ = 5.44 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1672790?version=3","version":3}