Measurement of nuclear effects on ψ(2S) production in p-Pb collisions at $$ \sqrt{s_{\mathrm{NN}}} $$ = 8.16 TeV

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<jats:title>A<jats:sc>bstract</jats:sc> </jats:title><jats:p>Inclusive <jats:italic>ψ</jats:italic>(2S) production is measured in p-Pb collisions at the centre-of-mass energy per nucleon-nucleon pair <jats:inline-formula><jats:alternatives><jats:tex-math>$$ \sqrt{s_{\mathrm{NN}}} $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msqrt> <mml:msub> <mml:mi>s</mml:mi> <mml:mi>NN</mml:mi> </mml:msub> </mml:msqrt> </mml:math></jats:alternatives></jats:inline-formula> = 8<jats:italic>.</jats:italic>16 TeV, using the ALICE detector at the CERN LHC. The production of <jats:italic>ψ</jats:italic>(2S) is studied at forward (2<jats:italic>.</jats:italic>03 <jats:italic>< y</jats:italic><jats:sub>cms</jats:sub><jats:italic><</jats:italic> 3<jats:italic>.</jats:italic>53) and backward (<jats:italic>−</jats:italic>4<jats:italic>.</jats:italic>46 <jats:italic>< y</jats:italic><jats:sub>cms</jats:sub><jats:italic>< −</jats:italic>2<jats:italic>.</jats:italic>96) centre-of-mass rapidity and for transverse momentum <jats:italic>p</jats:italic><jats:sub>T</jats:sub><jats:italic><</jats:italic> 12 GeV/<jats:italic>c</jats:italic> via the decay to muon pairs. In this paper, we report the integrated as well as the <jats:italic>y</jats:italic><jats:sub>cms</jats:sub>- and <jats:italic>p</jats:italic><jats:sub>T</jats:sub>-differential inclusive production cross sections. Nuclear effects on <jats:italic>ψ</jats:italic>(2S) production are studied via the determination of the nuclear modification factor that shows a strong suppression at both forward and backward centre-of-mass rapidities. Comparisons with corresponding results for inclusive J/<jats:italic>ψ</jats:italic> show a similar suppression for the two states at forward rapidity (p-going direction), but a stronger suppression for <jats:italic>ψ</jats:italic>(2S) at backward rapidity (Pb-going direction). As a function of <jats:italic>p</jats:italic><jats:sub>T</jats:sub>, no clear dependence of the nuclear modification factor is found. The relative size of nuclear effects on <jats:italic>ψ</jats:italic>(2S) production compared to J/<jats:italic>ψ</jats:italic> is also studied via the double ratio of production cross sections [<jats:italic>σ</jats:italic><jats:sub><jats:italic>ψ</jats:italic>(2S)</jats:sub><jats:italic>/σ</jats:italic><jats:sub>J<jats:italic>/ψ</jats:italic></jats:sub>]pPb<jats:italic>/</jats:italic>[<jats:italic>σ</jats:italic><jats:sub><jats:italic>ψ</jats:italic>(2S)</jats:sub><jats:italic>/σ</jats:italic><jats:sub>J<jats:italic>/ψ</jats:italic></jats:sub>]<jats:sub>pp</jats:sub> between p-Pb and pp collisions. The results are compared with theoretical models that include various effects related to the initial and final state of the collision system and also with previous measurements at <jats:inline-formula><jats:alternatives><jats:tex-math>$$ \sqrt{s_{\mathrm{NN}}} $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msqrt> <mml:msub> <mml:mi>s</mml:mi> <mml:mi>NN</mml:mi> </mml:msub> </mml:msqrt> </mml:math></jats:alternatives></jats:inline-formula> = 5<jats:italic>.</jats:italic>02 TeV.</jats:p>

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