{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.85626.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1692558"}},{"@id":"https://doi.org/10.1007/JHEP10(2018)138","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2019","description":"The differential yields of charged particles having pseudorapidity within $|\\eta|<$ 1 are measured using xenon-xenon (XeXe) collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.44 TeV. The data, corresponding to an integrated luminosity of 3.42 $\\mu$b$^{-1}$, were collected in 2017 by the CMS experiment at the LHC. The yields are reported as functions of collision centrality and transverse momentum, $p_\\mathrm{T}$, from 0.5 to 100 GeV. A previously reported $p_\\mathrm{T}$ spectrum from proton-proton collisions at $\\sqrt{s}$ = 5.02 TeV is used for comparison after correcting for the difference in center-of-mass energy. The nuclear modification factors using this reference, $R_\\mathrm{AA}^*$, are constructed and compared to previous measurements and theoretical predictions. In head-on collisions, the $R_\\mathrm{AA}^*$ has a value of 0.17 in the $p_\\mathrm{T}$ range of 6-8 GeV, but increases to approximately 0.7 at 100 GeV. Above $\\approx$ 6 GeV, the XeXe data show a notably smaller suppression than previous results for lead-lead (PbPb) collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.02 TeV when compared at the same centrality (i.e., the same fraction of total cross section). However, the XeXe suppression is slightly greater than that for PbPb in events having a similar number of participating nucleons.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.85626.v1/t1","@type":"Dataset","description":"The per-event differential invariant yield of charged particles having |eta|&lt;1 in XeXe collisions at sqrt(s_NN)=5.44 TeV. The first systematic uncertainty...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.85626.v1/t2","@type":"Dataset","description":"The per-event differential invariant yield of charged particles having |eta|&lt;1 in pp collisions at sqrt(s)=5.44 TeV, after extrpolation from 5.02...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.85626.v1/t3","@type":"Dataset","description":"The nuclear modification factor of charged particles having |eta|&lt;1 in XeXe collisions at sqrt(s_NN)=5.44 TeV. The first systematic uncertainty describes...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.85626.v1/t4","@type":"Dataset","description":"The nuclear modification factor of charged particles having |eta|&lt;1 in XeXe collisions at sqrt(s_NN)=5.44 TeV. The first systematic uncertainty describes...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.85626.v1/t5","@type":"Dataset","description":"The nuclear modification factor of charged particles having |eta|&lt;1 in XeXe collisions at sqrt(s_NN)=5.44 TeV. The first systematic uncertainty describes...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.85626.v1/t6","@type":"Dataset","description":"The RXePb of charged particles having |eta|&lt;1 in XeXe collisions at sqrt(s_NN)=5.44 TeV and PbPb collisions at sqrt(s_NN)=5.02 TeV. The...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.85626.v1/t7","@type":"Dataset","description":"The RXePb of charged particles having |eta|&lt;1 in XeXe collisions at sqrt(s_NN)=5.44 TeV and PbPb collisions at sqrt(s_NN)=5.02 TeV. The...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.85626.v1/t8","@type":"Dataset","description":"The RXePb of charged particles having |eta|&lt;1 in XeXe collisions at sqrt(s_NN)=5.44 TeV and PbPb collisions at sqrt(s_NN)=5.02 TeV. The...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.85626.v1/t9","@type":"Dataset","description":"The RXePb of charged particles having |eta|&lt;1 in XeXe collisions at sqrt(s_NN)=5.44 TeV and PbPb collisions at sqrt(s_NN)=5.02 TeV. The...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.85626.v1/t10","@type":"Dataset","description":"The average N_part, N_coll, and TAA for various centrality classes of XeXe collisions at 5.44 TeV.","name":"Table 10"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1692558?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/85626"}],"inLanguage":"en","name":"Charged-particle nuclear modification factors 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/ins1692558?version=1","version":1}