{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.75256.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1463284"}},{"@id":"https://doi.org/10.1016/j.physletb.2016.10.053","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2016","description":"CERN-LHC.  Measurements of the per-event charged-particle yield as a function of the charged-particle transverse momentum and rapidity are performed using $p+$Pb collision data collected by the ATLAS experiment at the LHC at a centre-of-mass energy of $\\sqrt{s_{NN}}=5.02$ TeV. Charged particles are reconstructed over pseudorapidity $|\\eta|&lt;2.3$ and transverse momentum between $0.1$ GeV and $22$ GeV in a dataset corresponding to an integrated luminosity of $1$ $\\mu b^{-1}$. The results are presented in the form of charged-particle nuclear modification factors, where the $p+$Pb charged-particle multiplicities are compared between central and peripheral $p+$Pb collisions as well as to charged-particle cross sections measured in pp collisions. The $p+$Pb collision centrality is characterized by the total transverse energy measured in $-4.9&lt;\\eta&lt;-3.1$, which is in the direction of the outgoing lead beam. Three different estimations of the number of nucleons participating in the $p+$Pb collision are carried out using the Glauber model and two Glauber-Gribov colour-fluctuation extensions to the Glauber model. The values of the nuclear modification factors are found to vary significantly as a function of rapidity and transverse momentum. A broad peak is observed for all centralities and rapidities in the nuclear modification factors for charged-particle transverse momentum values around $3$ GeV. The magnitude of the peak increases for more central collisions as well as rapidity ranges closer to the direction of the outgoing lead nucleus.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.75256.v1/t1","@type":"Dataset","description":"Invariant differential $p_{T}$ spectra of charged particles which are produced in p+Pb collisions at $\\sqrt{s_{NN}} = 5.02$ TeV shown in...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.75256.v1/t2","@type":"Dataset","description":"Invariant differential $p_{T}$ spectra of charged particles which are produced in p+Pb collisions at $\\sqrt{s_{NN}} = 5.02$ TeV shown in...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.75256.v1/t3","@type":"Dataset","description":"The invariant differential y* spectra of charged particles produced in p+Pb collisions at $\\sqrt{s_{NN}}=5.02$ TeV are shown in five centrality...","name":"Table 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