{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.88285.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1719334"}},{"@id":"https://doi.org/10.1016/j.physletb.2019.135049","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2019","description":"Measurements of the pseudorapidity distributions of charged hadrons produced in xenon-xenon collisions at a nucleon-nucleon centre-of-mass energy of $\\sqrt{s_\\mathrm{NN}} =$ 5.44 TeV are presented. The measurements are based on data collected by the CMS experiment at the LHC. The yield of primary charged hadrons produced in xenon-xenon collisions in the pseudorapidity range $|\\eta|$ $<$ 3.2 is determined using the silicon pixel detector in the CMS tracking system. For the 5% most central collisions, the charged-hadron pseudorapidity density in the midrapidity region $|\\eta|$ $<$ 0.5 is found to be 1187 $\\pm$ 36 (syst), with a negligible statistical uncertainty. The rapidity distribution of charged hadrons is also presented in the range $|y|$ $<$ 3.2 and is found to be independent of rapidity around $y =$ 0. Existing Monte-Carlo event generators are unable to simultaneously describe both results. Comparisons of charged-hadron multiplicities between xenon-xenon and lead-lead collisions at similar collision energies show that particle production at midrapidity is strongly dependent on the collision geometry in addition to the system size and collision energy.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.88285.v1/t1","@type":"Dataset","description":"Averaged and symmetrised charged-hadron pseudorapidity density distributions in XeXe collisions at $\\sqrt{s_{NN}} = 5.44$ TeV, for events in the 0--80\\%,...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.88285.v1/t2","@type":"Dataset","description":"Averaged and symmetrised charged-hadron rapidity density distributions in XeXe collisions at $\\sqrt{s_{NN}} = 5.44$ TeV, for events in the 0--80\\%...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.88285.v1/t3","@type":"Dataset","description":"Charged-hadron pseudorapidity density in XeXe collisions at $\\sqrt{s_{NN}} = 5.44$ TeV at midrapidity as a function of event centrality. The...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.88285.v1/t4","@type":"Dataset","description":"Charged-hadron pseudorapidity density in XeXe collisions at $\\sqrt{s_{NN}} = 5.44$ TeV at midrapidity, normalised by $2A$, where $A$ is the...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.88285.v1/t5","@type":"Dataset","description":"Average charged-hadron pseudorapidity density at midrapidity normalised by $\\langle N_{part} \\rangle$, shown as a function of $\\langle N_{part} \\rangle$. The...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.88285.v1/t6","@type":"Dataset","description":"Average charged-hadron pseudorapidity density at midrapidity normalised by $\\langle N_{part} \\rangle$, shown as a function of $\\langle N_{part} \\rangle/2A$, where...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.88285.v1/t7","@type":"Dataset","description":"Average charged-hadron pseudorapidity density at midrapidity normalised by $2A$, shown as a function of $\\langle N_{part} \\rangle/2A$, where $A$ is...","name":"Table 7"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1719334?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/88285"}],"inLanguage":"en","name":"Pseudorapidity distributions of charged hadrons in xenon-xenon 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/ins1719334?version=1","version":1}
