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| CMS-HIN-14-009 ; CERN-EP-2017-009 | ||
| Measurement of prompt and nonprompt $ \mathrm{J} / \psi $ production in pp and pPb collisions at $\sqrt{s_{\mathrm{NN}}} = $ 5.02 TeV | ||
| CMS Collaboration | ||
| 6 February 2017 | ||
| Eur. Phys. J. C 77 (2017) 269 | ||
| Abstract: This paper reports the measurement of $ \mathrm{J} / \psi $ meson production in proton-proton (pp) and proton-lead (pPb) collisions at a center-of-mass energy per nucleon pair of 5.02 TeV by the CMS experiment at the LHC. The data samples used in the analysis correspond to integrated luminosities of 28 pb$^{-1}$ and 35 nb$^{-1}$ for pp and pPb collisions, respectively. Prompt and nonprompt $ \mathrm{J} / \psi $ mesons, the latter issuing from the decay of B mesons, are measured in their dimuon decay channels. Differential cross sections are measured in the transverse momentum range of 2 $ < p_{\mathrm{T}} < $ 30 GeV/$c$, and center-of-mass rapidity ranges of $| {y_{\mathrm{CM}}} | < $ 2.4 (pp) and $-2.87 < y_{\mathrm{CM}} < 1.93 $ (pPb). The nuclear modification factor, $R_{{\mathrm{ p }\mathrm{Pb}} }$, is measured as functions of $p_{\mathrm{T}}$ and $y_{\mathrm{CM}}$. Small modifications of the $ \mathrm{J} / \psi $ cross sections are observed in pPb relative to pp collisions. The ratio of $ \mathrm{J} / \psi $ production cross sections in p-going and Pb-going directions, $R_{\mathrm{FB}}$, studied as functions of $p_{\mathrm{T}}$ and $y_{\mathrm{CM}}$, shows a significant decrease for increasing transverse energy deposited at large pseudorapidities. These results, which cover a wide kinematic range, provide new insight on the role of cold nuclear matter effects on prompt and nonprompt $ \mathrm{J} / \psi $ production. | ||
| Links: e-print arXiv:1702.01462 [nucl-ex] (PDF) ; CDS record ; inSPIRE record ; HepData record ; CADI line (restricted) ; | ||
| Figures & Tables | Summary | Additional Figures | References | CMS Publications |
|---|
| Figures | |
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Figure 1:
Examples of the invariant mass (left) and pseudo-proper decay length (right) distributions of $ \mu^{+} \mu^{-} $ pairs for pp (upper) and pPb (lower) collisions. The projections of the 2D fit function onto the respective axes are overlaid as solid lines. The long-dashed lines show the fitted contribution of nonprompt $ \mathrm{J} / \psi $ mesons. The fitted background contributions are shown by short-dashed lines. |
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Figure 1-a:
Invariant mass distribution of $ \mu^{+} \mu^{-} $ pairs for pp collisions. The projections of the 2D fit function onto the respective axes are overlaid as solid lines. The long-dashed lines show the fitted contribution of nonprompt $ \mathrm{J} / \psi $ mesons. The fitted background contributions are shown by short-dashed lines. |
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Figure 1-b:
Pseudo-proper decay length distribution of $ \mu^{+} \mu^{-} $ pairs for pp collisions. The projections of the 2D fit function onto the respective axes are overlaid as solid lines. The long-dashed lines show the fitted contribution of nonprompt $ \mathrm{J} / \psi $ mesons. The fitted background contributions are shown by short-dashed lines. |
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Figure 1-c:
Invariant mass distribution of $ \mu^{+} \mu^{-} $ pairs for Pb collisions. The projections of the 2D fit function onto the respective axes are overlaid as solid lines. The long-dashed lines show the fitted contribution of nonprompt $ \mathrm{J} / \psi $ mesons. The fitted background contributions are shown by short-dashed lines. |
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Figure 1-d:
Pseudo-proper decay length distribution of $ \mu^{+} \mu^{-} $ pairs for pPb collisions. The projections of the 2D fit function onto the respective axes are overlaid as solid lines. The long-dashed lines show the fitted contribution of nonprompt $ \mathrm{J} / \psi $ mesons. The fitted background contributions are shown by short-dashed lines. |
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Figure 2:
Differential cross section (multiplied by the dimuon branching fraction) of prompt $ \mathrm{J} / \psi $ mesons in pp (left) and pPb (right) collisions at forward (upper) and backward (lower) $ {y_{\mathrm {CM}}} $. The vertical bars (smaller than the symbols in most cases) represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty from the integrated luminosity determination, 2.3% for pp and 3.5% for pPb collisions, is not included in the point-by-point uncertainties. |
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Figure 2-a:
Differential cross section (multiplied by the dimuon branching fraction) of prompt $ \mathrm{J} / \psi $ mesons in pp collisions at forward $ {y_{\mathrm {CM}}} $. The vertical bars (smaller than the symbols in most cases) represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty from the integrated luminosity determination, 2.3%, is not included in the point-by-point uncertainties. |
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Figure 2-b:
Differential cross section (multiplied by the dimuon branching fraction) of prompt $ \mathrm{J} / \psi $ mesons in pPb collisions at forward $ {y_{\mathrm {CM}}} $. The vertical bars (smaller than the symbols in most cases) represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty from the integrated luminosity determination, 3.5%, is not included in the point-by-point uncertainties. |
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Figure 2-c:
Differential cross section (multiplied by the dimuon branching fraction) of prompt $ \mathrm{J} / \psi $ mesons in pp collisions at backward $ {y_{\mathrm {CM}}} $. The vertical bars (smaller than the symbols in most cases) represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty from the integrated luminosity determination, 2.3%, is not included in the point-by-point uncertainties. |
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Figure 2-d:
Differential cross section (multiplied by the dimuon branching fraction) of prompt $ \mathrm{J} / \psi $ mesons in pPb collisions at backward $ {y_{\mathrm {CM}}} $. The vertical bars (smaller than the symbols in most cases) represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty from the integrated luminosity determination, 3.5%, is not included in the point-by-point uncertainties. |
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Figure 3:
Rapidity dependence of the cross section (multiplied by the dimuon branching fraction) for prompt $ \mathrm{J} / \psi $ mesons in the $ {p_{\mathrm {T}}} $ intervals of 6.5 $ < {p_{\mathrm {T}}} < $ 10 GeV/$c$ (circles) and 10 $ < {p_{\mathrm {T}}} < $ 30 GeV/$c$ (squares) in pp (left) and pPb (right) collisions. The vertical dashed line indicates $ {y_{\mathrm {CM}}} = $ 0. The vertical bars (smaller than the symbols in most cases) represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty from the integrated luminosity determination, 2.3% for pp and 3.5% for pPb collisions, is not included in the point-by-point uncertainties. |
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Figure 3-a:
Rapidity dependence of the cross section (multiplied by the dimuon branching fraction) for prompt $ \mathrm{J} / \psi $ mesons in the $ {p_{\mathrm {T}}} $ intervals of 6.5 $ < {p_{\mathrm {T}}} < $ 10 GeV/$c$ (circles) and 10 $ < {p_{\mathrm {T}}} < $ 30 GeV/$c$ (squares) in pp collisions. The vertical dashed line indicates $ {y_{\mathrm {CM}}} = $ 0. The vertical bars (smaller than the symbols in most cases) represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty from the integrated luminosity determination, 2.3%, is not included in the point-by-point uncertainties. |
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Figure 3-b:
Rapidity dependence of the cross section (multiplied by the dimuon branching fraction) for prompt $ \mathrm{J} / \psi $ mesons in the $ {p_{\mathrm {T}}} $ intervals of 6.5 $ < {p_{\mathrm {T}}} < $ 10 GeV/$c$ (circles) and 10 $ < {p_{\mathrm {T}}} < $ 30 GeV/$c$ (squares) in pPb collisions. The vertical dashed line indicates $ {y_{\mathrm {CM}}} = $ 0. The vertical bars (smaller than the symbols in most cases) represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty from the integrated luminosity determination, 3.5%, is not included in the point-by-point uncertainties. |
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Figure 4:
Transverse momentum dependence of $ {R_{\mathrm{ p } \mathrm {Pb}}} $ for prompt $ \mathrm{J} / \psi $ mesons in seven $ {y_{\mathrm {CM}}} $ ranges. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty of 4.2% is displayed as a gray box at $ {R_{\mathrm{ p } \mathrm {Pb}}} = $ 1 next to the left axis. The predictions of shadowing models based on the parameterizations EPS09 and nCTEQ15 [14,46-48] are also shown. |
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Figure 5:
Rapidity dependence of $ {R_{\mathrm{ p } \mathrm {Pb}}} $ for prompt $ \mathrm{J} / \psi $ mesons in two $ {p_{\mathrm {T}}} $ ranges: 6.5 $ < {p_{\mathrm {T}}} < $ 10 GeV/$c$ (left) and 10 $ < {p_{\mathrm {T}}} < $ 30 GeV/$c$ (right). The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty of 4.2% is displayed as a gray box at $ {R_{\mathrm{ p } \mathrm {Pb}}} = $ 1 next to the left axis. The predictions of shadowing models based on the parameterizations EPS09 and nCTEQ15 [14,45,46,47] are also shown. |
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Figure 5-a:
Rapidity dependence of $ {R_{\mathrm{ p } \mathrm {Pb}}} $ for prompt $ \mathrm{J} / \psi $ mesons in $ {p_{\mathrm {T}}} $ range 6.5 $ < {p_{\mathrm {T}}} < $ 10 GeV/$c$. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty of 4.2% is displayed as a gray box at $ {R_{\mathrm{ p } \mathrm {Pb}}} = $ 1 next to the left axis. The predictions of shadowing models based on the parameterizations EPS09 and nCTEQ15 [14,46-48] are also shown. |
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Figure 5-b:
Rapidity dependence of $ {R_{\mathrm{ p } \mathrm {Pb}}} $ for prompt $ \mathrm{J} / \psi $ mesons in $ {p_{\mathrm {T}}} $ range 10 $ < {p_{\mathrm {T}}} < $ 30 GeV/$c$. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty of 4.2% is displayed as a gray box at $ {R_{\mathrm{ p } \mathrm {Pb}}} = $ 1 next to the left axis. The predictions of shadowing models based on the parameterizations EPS09 and nCTEQ15 [14,46-48] are also shown. |
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Figure 6:
Transverse momentum dependence of $ {R_{\mathrm {FB}}} $ for prompt $ \mathrm{J} / \psi $ mesons in three $ {y_{\mathrm {CM}}} $ regions. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. |
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Figure 6-a:
Transverse momentum dependence of $ {R_{\mathrm {FB}}} $ for prompt $ \mathrm{J} / \psi $ mesons in the 0 $ < {y_{\mathrm {CM}}} < $ 0.9 region. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. |
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Figure 6-b:
Transverse momentum dependence of $ {R_{\mathrm {FB}}} $ for prompt $ \mathrm{J} / \psi $ mesons in the 0.9 $ < {y_{\mathrm {CM}}} < $ 1.5 region. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. |
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Figure 6-c:
Transverse momentum dependence of $ {R_{\mathrm {FB}}} $ for prompt $ \mathrm{J} / \psi $ mesons in the 1.5 $ < {y_{\mathrm {CM}}} < $ 1.93 region. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. |
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Figure 7:
Dependence of $ {R_{\mathrm {FB}}} $ for prompt $ \mathrm{J} / \psi $ mesons on the hadronic activity in the event, given by the transverse energy deposited in the CMS detector at large pseudorapidities ${E_{\mathrm {T}}^{{\mathrm {HF}} {| \eta | }>4}} $. Data points are slightly shifted horizontally so that they do not overlap. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. |
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Figure 8:
Differential cross section (multiplied by the dimuon branching fraction) of nonprompt $ \mathrm{J} / \psi $ mesons in pp (left) and pPb (right) collisions at forward (upper) and backward (lower) $ {y_{\mathrm {CM}}} $. The vertical bars (smaller than the symbols in most cases) represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty from the integrated luminosity determination, 2.3% for pp and 3.5% for pPb collisions, is not included in the point-by-point uncertainties. |
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Figure 8-a:
Differential cross section (multiplied by the dimuon branching fraction) of nonprompt $ \mathrm{J} / \psi $ mesons in pp collisions at forward $ {y_{\mathrm {CM}}} $. The vertical bars (smaller than the symbols in most cases) represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty from the integrated luminosity determination, 2.3%, is not included in the point-by-point uncertainties. |
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Figure 8-b:
Differential cross section (multiplied by the dimuon branching fraction) of nonprompt $ \mathrm{J} / \psi $ mesons in pPb collisions at forward $ {y_{\mathrm {CM}}} $. The vertical bars (smaller than the symbols in most cases) represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty from the integrated luminosity determination, 3.5%, is not included in the point-by-point uncertainties. |
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Figure 8-c:
Differential cross section (multiplied by the dimuon branching fraction) of nonprompt $ \mathrm{J} / \psi $ mesons in pp collisions at backward $ {y_{\mathrm {CM}}} $. The vertical bars (smaller than the symbols in most cases) represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty from the integrated luminosity determination, 2.3%, is not included in the point-by-point uncertainties. |
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Figure 8-d:
Differential cross section (multiplied by the dimuon branching fraction) of nonprompt $ \mathrm{J} / \psi $ mesons in pPb collisions at backward $ {y_{\mathrm {CM}}} $. The vertical bars (smaller than the symbols in most cases) represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty from the integrated luminosity determination, 3.5%, is not included in the point-by-point uncertainties. |
png pdf |
Figure 9:
Rapidity dependence of the cross section (multiplied by the dimuon branching fraction) for nonprompt $ \mathrm{J} / \psi $ mesons in the $ {p_{\mathrm {T}}} $ intervals of 6.5 $ < {p_{\mathrm {T}}} < $ 10 GeV/$c$ (circles) and 10 $ < {p_{\mathrm {T}}} < $ 30 GeV/$c$ (squares) in pp (left) and pPb (right) collisions. The vertical dashed line indicates $ {y_{\mathrm {CM}}} = $ 0. The vertical bars (smaller than the symbols in most cases) represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty from the integrated luminosity determination, 2.3% for pp and 3.5% for pPb collisions, is not included in the point-by-point uncertainties. |
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Figure 9-a:
Rapidity dependence of the cross section (multiplied by the dimuon branching fraction) for nonprompt $ \mathrm{J} / \psi $ mesons in the $ {p_{\mathrm {T}}} $ intervals of 6.5 $ < {p_{\mathrm {T}}} < $ 10 GeV/$c$ (circles) and 10 $ < {p_{\mathrm {T}}} < $ 30 GeV/$c$ (squares) in pp collisions. The vertical dashed line indicates $ {y_{\mathrm {CM}}} = $ 0. The vertical bars (smaller than the symbols in most cases) represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty from the integrated luminosity determination, 2.3%, is not included in the point-by-point uncertainties. |
png pdf |
Figure 9-b:
Rapidity dependence of the cross section (multiplied by the dimuon branching fraction) for nonprompt $ \mathrm{J} / \psi $ mesons in the $ {p_{\mathrm {T}}} $ intervals of 6.5 $ < {p_{\mathrm {T}}} < $ 10 GeV/$c$ (circles) and 10 $ < {p_{\mathrm {T}}} < $ 30 GeV/$c$ (squares) in pPb collisions. The vertical dashed line indicates $ {y_{\mathrm {CM}}} = $ 0. The vertical bars (smaller than the symbols in most cases) represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty from the integrated luminosity determination, 3.5%, is not included in the point-by-point uncertainties. |
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Figure 10:
Transverse momentum dependence of $ {R_{\mathrm{ p } \mathrm {Pb}}} $ for nonprompt $ \mathrm{J} / \psi $ mesons in seven ${y_{\mathrm {CM}}}$ ranges. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty of 4.2% is displayed as a gray box at $ {R_{\mathrm{ p } \mathrm {Pb}}} = $ 1 next to the left axis. |
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Figure 11:
Rapidity dependence of $ {R_{\mathrm{ p } \mathrm {Pb}}} $ for nonprompt $ \mathrm{J} / \psi $ mesons in two $ {p_{\mathrm {T}}} $ ranges: 6.5 $ < {p_{\mathrm {T}}} < $ 10 GeV/$c$ (left) and 10 $ < {p_{\mathrm {T}}} < $ 30 GeV/$c$ (right). The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty of 4.2% is displayed as a gray box at $ {R_{\mathrm{ p } \mathrm {Pb}}} = $ 1 next to the left axis. |
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Figure 11-a:
Rapidity dependence of $ {R_{\mathrm{ p } \mathrm {Pb}}} $ for nonprompt $ \mathrm{J} / \psi $ mesons in $ {p_{\mathrm {T}}} $ range 6.5 $ < {p_{\mathrm {T}}} < $ 10 GeV/$c$. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty of 4.2% is displayed as a gray box at $ {R_{\mathrm{ p } \mathrm {Pb}}} = $ 1 next to the left axis. |
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Figure 11-b:
Rapidity dependence of $ {R_{\mathrm{ p } \mathrm {Pb}}} $ for nonprompt $ \mathrm{J} / \psi $ mesons in $ {p_{\mathrm {T}}} $ range 10 $ < {p_{\mathrm {T}}} < $ 30 GeV/$c$. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty of 4.2% is displayed as a gray box at $ {R_{\mathrm{ p } \mathrm {Pb}}} = $ 1 next to the left axis. |
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Figure 12:
Transverse momentum dependence of $ {R_{\mathrm {FB}}} $ for nonprompt $ \mathrm{J} / \psi $ mesons in three ${y_{\mathrm {CM}}}$ regions. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. |
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Figure 12-a:
Transverse momentum dependence of $ {R_{\mathrm {FB}}} $ for nonprompt $ \mathrm{J} / \psi $ mesons in the 0 < ${y_{\mathrm {CM}}}$ < 0.9 region. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. |
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Figure 12-b:
Transverse momentum dependence of $ {R_{\mathrm {FB}}} $ for nonprompt $ \mathrm{J} / \psi $ mesons in the 0.9 < ${y_{\mathrm {CM}}}$ < 1.5 region. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. |
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Figure 12-c:
Transverse momentum dependence of $ {R_{\mathrm {FB}}} $ for nonprompt $ \mathrm{J} / \psi $ mesons in the 1.5 < ${y_{\mathrm {CM}}}$ < 1.93 region. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. |
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Figure 13:
Dependence of $ {R_{\mathrm {FB}}} $ for nonprompt $ \mathrm{J} / \psi $ mesons on the hadronic activity in the event, given by the transverse energy deposited in the CMS detector at large pseudorapidities ${E_{\mathrm {T}}^{{\mathrm {HF}} {| \eta | }>4}} $. Data points are slightly shifted horizontally so that they do not overlap. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. |
| Tables | |
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Table 1:
Rapidity intervals and associated minimum $ {p_{\mathrm {T}}} $ values for the $ \mathrm{J} / \psi $ cross section measurements in pp and pPb collisions. |
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Table 2:
Ranges of forward transverse energy, ${E_{\mathrm {T}}^{{\mathrm {HF}} {| \eta | } > 4}} $, their mean values, and associated fractions of pPb events that fall into each category. |
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Table 3:
Summary of the relative systematic uncertainties for the cross section measurements, given in percentages, for prompt and nonprompt $ \mathrm{J} / \psi $ mesons in pp and pPb collisions. |
| Summary |
| Proton-proton (pp) and proton-lead (pPb) data at $\sqrt{s_{\mathrm{NN}}} = $ 5.02 TeV collected with the CMS detector are used to investigate the production of prompt and nonprompt $ \mathrm{J} / \psi $ mesons and their possible modifications due to cold nuclear matter effects. Double-differential cross sections, as well as the nuclear modification factor ${R_{\mathrm{ p }\mathrm{Pb}}}$ and forward-to-backward production ratio ${R_{\mathrm{FB}}} $, are reported as functions of the $ \mathrm{J} / \psi $ $ p_{\mathrm{T}} $ and $ {y_{\mathrm{CM}}} $. The ${R_{\mathrm{ p }\mathrm{Pb}}}$ values for prompt $ \mathrm{J} / \psi $ mesons are above unity in mid- and backward $ {y_{\mathrm{CM}}} $ intervals analyzed ($-2.4<{y_{\mathrm{CM}}} <0.9$), with a possible depletion in the most forward bin at low $p_{\mathrm{T}} \lesssim $ 7.5 GeV/$c$. In the case of nonprompt $ \mathrm{J} / \psi $ meson production, ${R_{\mathrm{ p }\mathrm{Pb}}}$ is compatible with unity in all $ {y_{\mathrm{CM}}} $ bins. The prompt $ \mathrm{J} / \psi $ ${R_{\mathrm{FB}}}$ is below unity for $p_{\mathrm{T}}\lesssim $ 7.5 GeV/$c$ and forward $| {{y_{\mathrm{CM}}} }| > $ 0.9, but is consistent with unity for $p_{\mathrm{T}} \gtrsim $ 10 GeV/$c$. For nonprompt $ \mathrm{J} / \psi $ mesons, ${R_{\mathrm{FB}}}$ tends to be below unity at $p_{\mathrm{T}} \lesssim $ 7.5 GeV/$c$ and increases for higher $ p_{\mathrm{T}} $, but with slightly larger uncertainties. The dependence of ${R_{\mathrm{FB}}}$ on the hadronic activity in pPb events has been studied through the variable ${E_{\mathrm{T}}^{{\mathrm{HF}}| {\eta} | > 4}} $, characterizing the transverse energy deposited in the CMS detector at large pseudorapidities 4 $ < | {\eta} | < $ 5.2. The ${R_{\mathrm{FB}}}$ ratio is observed to decrease with increasing event activity for both prompt and nonprompt $ \mathrm{J} / \psi $ mesons, indicating enhanced nuclear matter effects for increasingly central pPb collisions. A depletion of prompt $ \mathrm{J} / \psi $ mesons in pPb collisions (as compared to pp collisions) is expected in the forward $ {y_{\mathrm{CM}}} $ region because of the shadowing of nuclear parton distributions and/or coherent energy loss effects. Such a suppression is seen in the present data at ${y_{\mathrm{CM}}} > $ 1.5 and $p_{\mathrm{T}} \lesssim $ 7.5 GeV/$c$, but not at larger $ p_{\mathrm{T}} $, consistent with the expected reduced impact of nuclear parton distributions and coherent energy loss effects for increasing $ \mathrm{J} / \psi $ $ p_{\mathrm{T}} $. At negative $ {y_{\mathrm{CM}}} $, both shadowing and energy loss effects are known to lead to small nuclear modifications, as confirmed by the present measurements. Such processes are also expected to affect the nuclear dependence of B meson production and thereby, through its decays, the nonprompt $ \mathrm{J} / \psi $ production. The measurements presented here provide new constraints on cold nuclear matter effects on prompt and nonprompt $ \mathrm{J} / \psi $ production over a wide kinematic range. |
| Additional Figures | |
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Additional Figure 1:
$R_{\text {pPb}}$ vs. transverse momentum for $\mathrm{J}/\psi $ mesons measured in the forward rapidity region by the CMS (filled circles) and ALICE (open squares) [1] collaborations. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainties, 4% for the CMS and 6% for the ALICE results, are not included in the point-by-point uncertainties. |
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Additional Figure 2:
$R_{\text {pPb}}$ vs. transverse momentum for $\mathrm{J}/\psi $ mesons measured in the backward rapidity region by the CMS (filled circles) and ALICE (open squares) [1] collaborations. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainties, 4% for the CMS and 6% for the ALICE results, are not included in the point-by-point uncertainties. |
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Additional Figure 3:
$R_{\text {pPb}}$ vs. transverse momentum for prompt $\mathrm{J}/\psi $ mesons measured by the CMS (filled circles) and ATLAS (open squares) [2] collaborations. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainties of 4.2% for the CMS results is not included in the point-by-point uncertainties. |
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Additional Figure 4:
$R_{\text {pPb}}$ vs. rapidity for prompt $\mathrm{J}/\psi $ mesons measured by the CMS (filled circles) and ATLAS (open squares) [2] collaborations. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainties of 4.2% for the CMS results is not included in the point-by-point uncertainties. |
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Additional Figure 5:
$R_{\text {pPb}}$ vs. transverse momentum for nonprompt $\mathrm{J}/\psi $ mesons measured by the CMS (filled circles) and ATLAS (open squares) [2] collaborations. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainties of 4.2% for the CMS results is not included in the point-by-point uncertainties. |
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Additional Figure 6:
$R_{\text {pPb}}$ vs. rapidity for nonprompt $\mathrm{J}/\psi $ mesons measured by the CMS (filled circles) and ATLAS (open squares) [2] collaborations. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainties of 4.2% for the CMS results is not included in the point-by-point uncertainties. |
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Additional Figure 7:
$R_{\text {pPb}}$ vs. transverse momentum for nonprompt $\mathrm{J}/\psi $ (filled circles) and B$^+$ mesons (open squares) [3] measured by the CMS collaboration. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainties, 2.3% from pp integrated luminosity determination for nonprompt $\mathrm{J}/\psi $ results, 3.5% from pPb integrated luminosity determination, and 3.1% from B$^{+}$ meson branching fraction, are not included in the point-by-point uncertainties. |
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Additional Figure 8:
$R_{\text {pPb}}$ vs. rapidity for nonprompt $\mathrm{J}/\psi $ (filled circles) and B$^+$ mesons (open squares) [3] measured by the CMS collaboration. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainties, 2.3% from pp integrated luminosity determination for nonprompt $\mathrm{J}/\psi $ results, 3.5% from pPb integrated luminosity determination, and 3.1% from B$^{+}$ meson branching fraction, are not included in the point-by-point uncertainties. |
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Additional Figure 9:
$ {R_{\text {FB}}} $ vs. transverse momentum for $\mathrm{J}/\psi $ mesons measured in the forward rapidity region by the CMS (filled circles), LHCb (open squares) [4], and ALICE (open diamonds) [5] collaborations. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. |
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Additional Figure 10:
$ {R_{\text {FB}}} $ vs. rapidity for $\mathrm{J}/\psi $ mesons measured by the CMS (filled circles and squares), ATLAS (open crosses) [6], LHCb (open squares) [4], and ALICE (open diamonds) [5] collaborations. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. |
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Additional Figure 11:
$ {R_{\text {FB}}} $ vs. transverse momentum for nonprompt $\mathrm{J}/\psi $ mesons measured in the forward rapidity region by the CMS (filled circles) and LHCb (open squares) [4] collaborations. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. |
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Additional Figure 12:
$ {R_{\text {FB}}} $ vs. rapidity for nonprompt $\mathrm{J}/\psi $ mesons measured the CMS (filled circles and squares), ATLAS (open crosses) [6], and LHCb (open squares) [4] collaborations. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. |
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Additional Figure 13:
$R_{\text {pPb}}$ vs. transverse momentum for prompt $\mathrm{J}/\psi $ mesons. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty of 4.2% is displayed as a gray box at $R_{\text {pPb}}=$ 1 next to the left axis. |
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Additional Figure 14:
$R_{\text {pPb}}$ vs. rapidity for prompt $\mathrm{J}/\psi $ mesons in 6.5 $ < p_{\mathrm {T}} < $ 10 GeV/$c$. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty of 4.2% is displayed as a gray box at $R_{\text {pPb}}=$ 1 next to the left axis. |
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Additional Figure 15:
$R_{\text {pPb}}$ vs. rapidity for prompt $\mathrm{J}/\psi $ mesons in 10 $ < p_{\mathrm {T}} < $ 30 GeV/$c$. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty of 4.2% is displayed as a gray box at $R_{\text {pPb}}= $ 1 next to the left axis. |
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Additional Figure 16:
$R_{\text {pPb}}$ vs. transverse momentum for prompt $\mathrm{J}/\psi $ mesons integrated over $|y_{\text {CM}}|< $ 1.93. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty of 4.2% is displayed as a gray box at $R_{\text {pPb}}= $ 1 next to the left axis. |
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Additional Figure 17:
$R_{\text {pPb}}$ vs. transverse momentum for nonprompt $\mathrm{J}/\psi $ mesons integrated over $|y_{\text {CM}}|< $ 1.93. The vertical bars represent the statistical uncertainties and the shaded boxes show the systematic uncertainties. The fully correlated global uncertainty of 4.2% is displayed as a gray box at $R_{\text {pPb}}= $ 1 next to the left axis. |
| References | ||||
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