At intermediate transverse momentum (hmlsrc">hImg" 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/chContainer hidden">hCode">h altimg="si108.gif" overflow="scroll">2<phvariant="normal">T<10 GeVhy="false">/ch>) the proton-to-pion ratio increases with multiplicity in p–Pb collisions, a similar effect is not present in the kaon-to-pion ratio. The hmlsrc">hImg" 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">pThContainer hidden">hCode">h altimg="si3.gif" overflow="scroll">phvariant="normal">Th> dependent structure of such increase is qualitatively similar to those observed in pp and heavy-ion collisions. At high hmlsrc">hImg" 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">pThContainer hidden">hCode">h altimg="si3.gif" overflow="scroll">phvariant="normal">Th> (hmlsrc">hImg" 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/chContainer hidden">hCode">h altimg="si8.gif" overflow="scroll">>10 GeVhy="false">/ch>), the particle ratios are consistent with those reported for pp and Pb–Pb collisions at the LHC energies.
At intermediate hmlsrc">hImg" 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">pThContainer hidden">hCode">h altimg="si3.gif" overflow="scroll">phvariant="normal">Th> the (anti)proton hmlsrc">hImg" 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">RpPbhContainer hidden">hCode">h altimg="si6.gif" overflow="scroll">Rhvariant="normal">pPbh> shows a Cronin-like enhancement, while pions and kaons show little or no nuclear modification. At high hmlsrc">hImg" 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">pThContainer hidden">hCode">h altimg="si3.gif" overflow="scroll">phvariant="normal">Th> the charged pion, kaon and (anti)proton hmlsrc">hImg" 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">RpPbhContainer hidden">hCode">h altimg="si6.gif" overflow="scroll">Rhvariant="normal">pPbh> are consistent with unity within statistical and systematic uncertainties.