CMS-HIN-12-009 ; CERN-EP-2016-098 | ||
Coherent $\mathrm{ J } / \psi $ photoproduction in ultra-peripheral PbPb collisions at $\sqrt{s_{ \mathrm{NN}}} = $ 2.76 TeV with the CMS experiment | ||
CMS Collaboration | ||
23 May 2016 | ||
Phys. Lett. B 772 (2017) 489 | ||
Abstract: The cross section for coherent $\mathrm{ J } / \psi$ photoproduction accompanied by at least one neutron on one side of the interaction point and no neutron activity on the other side, $X_{\mathrm{n}}0_{\mathrm{n}}$, is measured with the CMS experiment in ultra-peripheral PbPb collisions at $\sqrt{s_{ \mathrm{NN}}} = $ 2.76 TeV. The analysis is based on a data sample corresponding to an integrated luminosity of 159 $\mu$b$^{-1}$, collected during the 2011 PbPb run. The $\mathrm{ J } / \psi$ mesons are reconstructed in the dimuon decay channel, while neutrons are detected using zero degree calorimeters. The measured cross section is $\mathrm{d}\sigma^{\text{coh}}_{X_{\mathrm{n}}0_{\mathrm{n}}}/{\mathrm{d} y}( \mathrm{ J } / \psi ) =$ 0.36 $\pm$ 0.04 (stat) $\pm$ 0.04 (syst) mb in the rapidity interval 1.8 $ < |{y}| < $ 2.3 . Using a model for the relative rate of coherent photoproduction processes, this $X_{\mathrm{n}}0_{\mathrm{n}}$ measurement gives a total coherent photoproduction cross section of ${\mathrm{d}\sigma^{\text{coh}}}/{\mathrm{d} y}( \mathrm{ J } / \psi ) =$ 1.82 $\pm$ 0.22 (stat) $\pm$ 0.20 (syst) $\pm$ 0.19 (theo) mb. The data strongly disfavour the impulse approximation model prediction, indicating that nuclear effects are needed to describe coherent $\mathrm{ J } / \psi$ photoproduction in $\gamma $+Pb interactions. The data are found to be consistent with the leading twist approximation, which includes nuclear gluon shadowing. | ||
Links: e-print arXiv:1605.06966 [nucl-ex] (PDF) ; CDS record ; inSPIRE record ; CADI line (restricted) ; |
Figures | |
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Figure 1-a:
Results from the simultaneous fit to dimuon invariant mass (a) and $ {p_{\mathrm {T}}} $ (b) distributions from opposite-sign muon pairs with $ {p_{\mathrm {T}}} < $ 1.0 GeV, 1.8 $ < {| y | }< $ 2.3 and 2.6 $ |
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Figure 1-b:
Results from the simultaneous fit to dimuon invariant mass (a) and $ {p_{\mathrm {T}}} $ (b) distributions from opposite-sign muon pairs with $ {p_{\mathrm {T}}} < $ 1.0 GeV, 1.8 $ < {| y | }< $ 2.3 and 2.6 $ |
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Figure 2:
Differential cross section versus rapidity for coherent $ {\mathrm{ J } / \psi } $ production in ultra-peripheral PbPb collisions at $\sqrt {s_{ \mathrm{NN}}}= $ 2.76 TeV , measured by ALICE [29,30] and CMS (see text for details). The vertical error bars include the statistical and systematic uncertainties added in quadrature, and the horizontal bars represent the range of the measurements in $y$. Also the impulse approximation and the leading twist approximation calculations are shown (see text for details). |
Tables | |
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Table 1:
Summary of systematic uncertainties for coherent $ {\mathrm{ J } / \psi } $ events in the $ {X_{\mathrm {n}}0_{\mathrm {n}}} $ configuration. |
Summary |
The coherent $\mathrm{ J } / \psi$ photoproduction cross section in ultra-peripheral PbPb collisions at $\sqrt{s_{ \mathrm{NN}}} =$ 2.76 TeV, in conjunction with at least one neutron on one side of the interaction point and no neutron activity on the other side, is measured to be ${\mathrm{d}\sigma^{\text{coh}}_{X_{\mathrm{n}}0_{\mathrm{n}}}}/{\mathrm{d} y}( \mathrm{ J } / \psi ) =$ 0.36 $\pm$ 0.04 (stat) $\pm$ 0.04 (syst) mb in the rapidity interval 1.8 $ < |{y}| < $ 2.3 . This measurement is extrapolated to the total coherent $\mathrm{ J } / \psi$ cross section, resulting in ${\mathrm{d}\sigma^{\text{coh}}}/{\mathrm{d} y}( \mathrm{ J } / \psi ) =$ 1.82 $\pm$ 0.22 (stat) $\pm$ 0.20 (syst) $\pm$ 0.19 (theo) mb in the measured rapidity interval. These results complement recent measurements on coherent $\mathrm{ J } / \psi$ photoproduction in ultra-peripheral PbPb collisions at $\sqrt{s_{ \mathrm{NN}}} =$ 2.76 TeV by the ALICE collaboration. An impulse approximation model prediction is strongly disfavored, indicating that nuclear effects expected to be present at low $x$ and $Q^2$ values are needed to describe the data. The prediction given by the leading twist approximation, which includes nuclear gluon shadowing, is consistent with the data. |
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Compact Muon Solenoid LHC, CERN |