{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.58980.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1088823"}},{"@id":"https://doi.org/10.1140/epjc/s10052-012-1945-x","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2012","description":"CERN-LHC.  Measurements of the transverse momentum spectra of charged particles produced in Lead-Lead nuclei collisions at a centre-of-mass energy per nucleon of 2.76 TeV. The measurements use data sets collected in  2010 and 2011 with respective integrated luminosities of 7 mub-1 and 150 mub-1, covering the PT range up to 100 GeV. A reference measurement  uses proton-proton data at centre-of-mass energy 2.76 TeV  collected in 2011 with integrated luminosity 230 nb-1. Particle yields and invariant differential spectra are presented in a variety of centrality ranges from 0-90%, together with the nuclear modification factor RAA and  the TAA-scaled ratios between central and peripheral centrality regions.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.58980.v1/t1","@type":"Dataset","description":"Invariant charged particle differential yields for |eta|<1.0 for P P collisions.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.58980.v1/t2","@type":"Dataset","description":"Inclusive scaled charged particle invariant cross section.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.58980.v1/t3","@type":"Dataset","description":"Invariant charged particle differential yield in the centrality regions 0 TO 5%, 5 TO 10% and 10 TO 30%.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.58980.v1/t4","@type":"Dataset","description":"Invariant charged particle differential yield in the centrality regions 30 TO 50%, 50 TO 70% and 70 TO 90%.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.58980.v1/t5","@type":"Dataset","description":"Nuclear modification factor RAA in the centrality regions 0 TO 5%, 5 TO 10% and 10 TO 30%.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.58980.v1/t6","@type":"Dataset","description":"Nuclear modification factor RAA in the centrality regions 30 TO 50%, 50 TO 70% and 70 TO 90%.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.58980.v1/t7","@type":"Dataset","description":"TAA-scaled ratio of PT spectra in central and peripheral bins, RCP.","name":"Table 7"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1088823?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/58980"}],"inLanguage":"en","name":"Study of high-pT charged particle suppression in PbPb compared to pp collisions at sqrt(sNN)=2.76 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1088823?version=1","version":1}