{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.128138.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1856529"}},{"@id":"https://doi.org/10.1016/j.physletb.2022.136943","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2022","description":"CERN-LHC. Neutral pion and ETA meson production cross sections were measured up to unprecedentedly high transverse momenta ($p_\\mbox{T}$) in p-Pb collisions at $\\sqrt{s_\\mbox{NN}}=8.16$ TeV. The mesons were reconstructed via their two-photon decay channel in the rapidity interval $-1.3<y_\\mbox{cms}<0.3$ in the ranges of $0.4<p_\\mbox{T}<200$ GeV/$c$ and $1.0<p_\\mbox{T}<50$ GeV/$c$, respectively. The respective nuclear modification factor ($R_\\mbox{pPb}$) is presented for $p_\\mbox{T}$ up to of 200 and 30 GeV/$c$, where the former was achieved extending the PI0 measurement in pp collisions at $\\sqrt{s}=8$ TeV. The values of $R_\\mbox{pPb}$ are below unity for $p_\\mbox{T}<10$ GeV/$c$, while they are consistent with unity for $p_\\mbox{T}>10$ GeV/$c$, leaving essentially no room for final state energy loss. The new data provide constraints for nuclear parton distribution and fragmentation functions over a broad kinematic range and are compared to model predictions as well as previous results at $\\sqrt{s_\\mbox{NN}}=5.02$ TeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.128138.v1/t1","@type":"Dataset","description":"Invariant differential cross section of PI0 produced in inelastic p-Pb collisions at a centre-of-mass energy per nucleon of 8.16 TeV,...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.128138.v1/t2","@type":"Dataset","description":"Invariant differential cross section of PI0 produced in inelastic pp collisions at a centre-of-mass energy of 8 TeV, the uncertainty...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.128138.v1/t3","@type":"Dataset","description":"Invariant differential cross section of ETA produced in inelastic p-Pb collisions at a centre-of-mass energy per nucleon of 8.16 TeV,...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.128138.v1/t4","@type":"Dataset","description":"Invariant differential cross section of ETA produced in inelastic pp collisions at a centre-of-mass energy of 8 TeV, the uncertainty...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.128138.v1/t5","@type":"Dataset","description":"The measured ratio of cross sections for inclusive ETA to PI0 production in inelastic p-Pb collisions at a centre-of-mass energy...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.128138.v1/t6","@type":"Dataset","description":"The measured ratio of cross sections for inclusive ETA to PI0 production in inelastic pp collisions at a centre-of-mass energy...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.128138.v1/t7","@type":"Dataset","description":"The nuclear modification factor RPPB of PI0 as a function of pT in inelastic p-Pb collisions at a centre-of-mass energy...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.128138.v1/t8","@type":"Dataset","description":"The nuclear modification factor RPPB of ETA as a function of pT in inelastic p-Pb collisions at a centre-of-mass energy...","name":"Table 8"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1856529?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/128138"}],"inLanguage":"en","name":"Nuclear modification factor of light neutral-meson spectra up to high transverse momentum in p-Pb collisions at $\\sqrt{s_{NN}}$ = 8.16 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1856529?version=1","version":1}