Abstract

The inclusive production of the $\psi$(2S) charmonium state was studied as a function of centrality in p-Pb collisions at the nucleon-nucleon center of mass energy $\sqrt{s_{\rm NN}}$ = 5.02 TeV at the CERN LHC. The measurement was performed with the ALICE detector in the center of mass rapidity ranges $-4.46<y_{\rm cms}<-2.96$ and $2.03<y_{\rm cms}<3.53$, down to zero transverse momentum, by reconstructing the $\psi$(2S) decay to a muon pair. The $\psi$(2S) production cross section $\sigma_{\psi(\rm 2S)}$ is presented as a function of the collision centrality, which is estimated through the energy deposited in forward rapidity calorimeters. The relative strength of nuclear effects on the $\psi$(2S) and on the corresponding 1S charmonium state J/$\psi$ is then studied by means of the double ratio of cross sections $[\sigma_{\psi(\rm 2S)}/\sigma_{\rm J/\psi}]_{\rm pPb}/[\sigma_{\psi(\rm 2S)}/\sigma_{\rm J/\psi}]_{\rm pp}$ between p-Pb and pp collisions, and by the values of the nuclear modification factors for the two charmonium states. The results show a large suppression of $\psi$(2S) production relative to the J/$\psi$ at backward (negative) rapidity, corresponding to the flight direction of the Pb-nucleus, while at forward (positive) rapidity the suppressions of the two states are comparable. Finally, comparisons to results from lower energy experiments and to available theoretical models are presented.

Highlights

  • The ψ(2S) production cross section σψ(2S) is presented as a function of the collision centrality, which is estimated through the energy deposited in forward rapidity calorimeters

  • Coherent energy loss mechanisms [6], have a similar effect on the two resonances, due to the fact that they act on a compact cc pair not yet evolved into a final color singlet state

  • In order to vary the thickness of CNM crossed by the cc pair, one can rather select classes of events based on estimators of the geometry of the collision, corresponding to various ranges in the number of nucleon-nucleon collisions Ncoll

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Summary

Experimental conditions

The analysis presented in this Letter is based on the detection of the ψ(2S) → μ+μ− decay in the forward muon spectrometer of ALICE, described in detail elsewhere [28, 29]. This detector covers the pseudorapidity range −4 < ηlab < −2.5 and includes a 3 T· m dipole magnet and five stations of tracking chambers, the central one being inside the magnet gap. A second absorber is placed downstream of the tracking detectors It removes the remaining hadrons and low-momentum muons produced predominantly from π and K decays, and is followed by two stations of trigger chambers that select muon candidates based on their transverse momentum (pT). The covered dimuon rapidity ranges were 2.03 < ycms < 3.53 and −4.46 < ycms < −2.96 for the p-Pb and Pb-p configurations, respectively

Data analysis
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