Multiplicity dependence of charged pion, kaon, and (anti)proton production at large transverse momentum in p-Pb collisions at
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The production of charged pions, kaons and (anti)protons has been measured at mid-rapidity (data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303914&_mathId=si2.gif&_user=111111111&_pii=S0370269316303914&_rdoc=1&_issn=03702693&md5=a6bcb7b69469d31dc0318f66fec13f58" title="Click to view the MathML source">−0.5<y<0) in p&ndash;Pb collisions at data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303914&_mathId=si1.gif&_user=111111111&_pii=S0370269316303914&_rdoc=1&_issn=03702693&md5=1c2ae747013ad8d2a2bc1ccb56bc8b85">View the MathML sourcedata-inlimgeid="1-s2.0-S0370269316303914-si1.gif"> using the ALICE detector at the LHC. Exploiting particle identification capabilities at high transverse momentum (data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303914&_mathId=si3.gif&_user=111111111&_pii=S0370269316303914&_rdoc=1&_issn=03702693&md5=13414abcb31dd6dbfab981dd0084def3" title="Click to view the MathML source">pT), the previously published data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303914&_mathId=si3.gif&_user=111111111&_pii=S0370269316303914&_rdoc=1&_issn=03702693&md5=13414abcb31dd6dbfab981dd0084def3" title="Click to view the MathML source">pT spectra have been extended to include measurements up to 20 GeV/c   for seven event multiplicity classes. The data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303914&_mathId=si3.gif&_user=111111111&_pii=S0370269316303914&_rdoc=1&_issn=03702693&md5=13414abcb31dd6dbfab981dd0084def3" title="Click to view the MathML source">pT spectra for pp collisions at data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303914&_mathId=si11.gif&_user=111111111&_pii=S0370269316303914&_rdoc=1&_issn=03702693&md5=0e57ad0bb248f456bc87959bd0554927">View the MathML sourcedata-inlimgeid="1-s2.0-S0370269316303914-si11.gif">, needed to interpolate a pp reference spectrum, have also been extended up to 20 GeV/c   to measure the nuclear modification factor (data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303914&_mathId=si6.gif&_user=111111111&_pii=S0370269316303914&_rdoc=1&_issn=03702693&md5=bb93f544fc6743d67eb3ca7cb0ea856a" title="Click to view the MathML source">RpPb) in non-single diffractive p&ndash;Pb collisions.

At intermediate transverse momentum (data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303914&_mathId=si108.gif&_user=111111111&_pii=S0370269316303914&_rdoc=1&_issn=03702693&md5=9f4f6878d76df75bc68ca19a9ddb846a" title="Click to view the MathML source">2<pT<10 GeV/c) the proton-to-pion ratio increases with multiplicity in p&ndash;Pb collisions, a similar effect is not present in the kaon-to-pion ratio. The data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303914&_mathId=si3.gif&_user=111111111&_pii=S0370269316303914&_rdoc=1&_issn=03702693&md5=13414abcb31dd6dbfab981dd0084def3" title="Click to view the MathML source">pT dependent structure of such increase is qualitatively similar to those observed in pp and heavy-ion collisions. At high data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303914&_mathId=si3.gif&_user=111111111&_pii=S0370269316303914&_rdoc=1&_issn=03702693&md5=13414abcb31dd6dbfab981dd0084def3" title="Click to view the MathML source">pT (data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303914&_mathId=si8.gif&_user=111111111&_pii=S0370269316303914&_rdoc=1&_issn=03702693&md5=d0ca309d8ec4199226ff18fec4a5eeb6" title="Click to view the MathML source">>10 GeV/c), the particle ratios are consistent with those reported for pp and Pb&ndash;Pb collisions at the LHC energies.

At intermediate data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303914&_mathId=si3.gif&_user=111111111&_pii=S0370269316303914&_rdoc=1&_issn=03702693&md5=13414abcb31dd6dbfab981dd0084def3" title="Click to view the MathML source">pT the (anti)proton data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303914&_mathId=si6.gif&_user=111111111&_pii=S0370269316303914&_rdoc=1&_issn=03702693&md5=bb93f544fc6743d67eb3ca7cb0ea856a" title="Click to view the MathML source">RpPb shows a Cronin-like enhancement, while pions and kaons show little or no nuclear modification. At high data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303914&_mathId=si3.gif&_user=111111111&_pii=S0370269316303914&_rdoc=1&_issn=03702693&md5=13414abcb31dd6dbfab981dd0084def3" title="Click to view the MathML source">pT the charged pion, kaon and (anti)proton data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316303914&_mathId=si6.gif&_user=111111111&_pii=S0370269316303914&_rdoc=1&_issn=03702693&md5=bb93f544fc6743d67eb3ca7cb0ea856a" title="Click to view the MathML source">RpPb are consistent with unity within statistical and systematic uncertainties.

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