Study of $J/\psi$ production and cold nuclear matter effects in $p$Pb collisions at $\sqrt{s_{NN}}$ = 5 TeV

Information

LHCb-PAPER-2013-052
CERN-PH-EP-2013-156
arXiv:1308.6729 [PDF]

(Submitted on 30 Aug 2013)
JHEP 02 (2014) 72
Inspire 1251899

Tools

Abstract

The production of $J/\psi$ mesons with rapidity $1.5<y<4.0$ or $-5.0<y<-2.5$ and transverse momentum $p_\mathrm{T}<14 \mathrm{GeV}/c$ is studied with the LHCb detector in proton-lead collisions at a nucleon-nucleon centre-of-mass energy $\sqrt{s_{NN}}=5 \mathrm{TeV}$. The analysis is based on a data sample corresponding to an integrated luminosity of about $1.6 \mathrm{nb}^{-1}$. For the first time the nuclear modification factor and forward-backward production ratio are determined separately for prompt $J/\psi$ mesons and $J/\psi$ from $b$-hadron decays. Clear suppression of prompt $J/\psi$ production with respect to proton-proton collisions at large rapidity is observed, while the production of $J/\psi$ from $b$-hadron decays is less suppressed. These results show good agreement with available theoretical predictions. The measurement shows that cold nuclear matter effects are important for interpretations of the related quark-gluon plasma signatures in heavy-ion collisions.

Figures and captions

Projections of the combined fit on (a, b) dimuon invariant mass and (c, d) $t_z$ in two representative bins in the (a, c) forward and (b, d) backward samples. For the mass projections the (red solid curve) total fitted function is shown together with the (blue dotted curve) $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ signal and (green dotted curve) background contributions. For the $t_z$ projections the total fitted function is indicated by the solid red curve, the background by the green hatched area, the prompt signal by the blue area and $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ from $b$ by the solid black curve.	Fig1a.pdf [20 KiB] HiDef png [249 KiB] Thumbnail [230 KiB] *.C file
	Fig1b.pdf [20 KiB] HiDef png [250 KiB] Thumbnail [236 KiB] *.C file
	Fig1c.pdf [23 KiB] HiDef png [428 KiB] Thumbnail [288 KiB] *.C file
	Fig1d.pdf [23 KiB] HiDef png [455 KiB] Thumbnail [303 KiB] *.C file
Distributions (normalised to unitary integral) of (a) track multiplicity and the $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ (b) transverse momentum $p_\mathrm{T}$, (c) momentum $p$, and (d) rapidity in laboratory frame $y_{\mathrm{lab}}$ in (black dots) forward and (red squares) backward regions of $ p\mathrm{Pb} $ collisions, and in (blue triangles) simulated $pp$ collisions. The distributions are background subtracted using the sPlot technique.	Fig2a.pdf [15 KiB] HiDef png [143 KiB] Thumbnail [155 KiB] *.C file
	Fig2b.pdf [17 KiB] HiDef png [178 KiB] Thumbnail [174 KiB] *.C file
	Fig2c.pdf [17 KiB] HiDef png [194 KiB] Thumbnail [196 KiB] *.C file
	Fig2d.pdf [17 KiB] HiDef png [166 KiB] Thumbnail [161 KiB] *.C file
Single differential production cross-sections for (black dots) prompt $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ and (red squares) $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ from $b$ as functions of (a, b) $p_\mathrm{T}$ and (c, d) $y$ in the (a, c) forward and (b, d) backward regions.	Fig3a.pdf [14 KiB] HiDef png [123 KiB] Thumbnail [142 KiB] *.C file
	Fig3b.pdf [15 KiB] HiDef png [129 KiB] Thumbnail [146 KiB] *.C file
	Fig3c.pdf [14 KiB] HiDef png [137 KiB] Thumbnail [159 KiB] *.C file
	Fig3d.pdf [14 KiB] HiDef png [139 KiB] Thumbnail [161 KiB] *.C file
Double differential production cross-sections for (a) prompt $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ mesons and (b) $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ from $b$ in the forward samples.	Fig4a.pdf [16 KiB] HiDef png [173 KiB] Thumbnail [179 KiB] *.C file
	Fig4b.pdf [17 KiB] HiDef png [184 KiB] Thumbnail [183 KiB] *.C file
Nuclear modification factor $R_{ p\mathrm{Pb} }$ as a function of $y$ for (a) prompt $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ mesons and (b) $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ from $b$, together with the theoretical predictions from (yellow dashed line and brown band) Refs. \cite{Ferreiro:2013pua,delValle:2014wha}, (blue band) Ref. \cite{Albacete:2013ei}, and (green solid and blue dash-dotted lines) Ref. \cite{Arleo:2012rs}. The inner error bars (delimited by the horizontal lines) show the statistical uncertainties; the outer ones show the statistical and systematic uncertainties added in quadrature. The uncertainty due to the interpolated $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ cross-section in $pp$ collisions at $\sqrt{s}=5\mathrm{ Te V} $ is $5.5\%$ ($8.4\%$) for prompt $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ mesosns ($ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ from $b$).	Fig5a.pdf [16 KiB] HiDef png [700 KiB] Thumbnail [332 KiB] *.C file
	Fig5b.pdf [14 KiB] HiDef png [460 KiB] Thumbnail [245 KiB] *.C file
Forward-backward production ratio $R_{ {FB}}$ as a function of $\|y\|$ for (a) prompt $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ mesons and (b) $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ from $b$, together with the theoretical predictions from (yellow dashed line and brown band) Refs. \cite{Ferreiro:2013pua,delValle:2014wha}, (blue band) Ref. \cite{Albacete:2013ei}, and (green solid and blue dash-dotted lines) Ref. \cite{Arleo:2012rs}. The inner error bars (delimited by the horizontal lines) show the statistical uncertainties; the outer ones show the statistical and systematic uncertainties added in quadrature.	Fig6a.pdf [15 KiB] HiDef png [844 KiB] Thumbnail [372 KiB] *.C file
	Fig6b.pdf [14 KiB] HiDef png [738 KiB] Thumbnail [341 KiB] *.C file
Forward-backward production ratio $R_{ {FB}}$ for (black dot) prompt $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ mesons and (red square) $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ from $b$ as a function of $p_\mathrm{T}$ in the rapidity range $2.5<\|y\|<4.0$. The theoretical predictions from (blue band) Ref. \cite{Albacete:2013ei} and (green solid and blue dash-dotted lines) Ref. \cite{Arleo:2013zua} are for prompt $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} $ mesons. The inner error bars (delimited by the horizontal lines) show the statistical uncertainties; the outer ones show the statistical and systematic uncertainties added in quadrature.	Fig7.pdf [17 KiB] HiDef png [234 KiB] Thumbnail [209 KiB] *.C file
Animated gif made out of all figures.	PAPER-2013-052.gif Thumbnail

Tables and captions

Relative systematic uncertainties on the differential production cross-sections. The uncertainty due to the radiative tail and branching fraction cancels in both $R_{ p\mathrm{Pb} }$ and $R_{ {FB}}$. The uncertainty due to the tracking efficiency and the luminosity partially cancels for $R_{ {FB}}$.	Table_1.pdf [67 KiB] HiDef png [94 KiB] Thumbnail [42 KiB] tex code
Single differential production cross-sections (in $ {\rm \upmu b} /( {\mathrm{ Ge V /}c} )$) for prompt $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu}$ mesons and $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu}$ from $b$ as functions of transverse momentum. The first uncertainty is statistical, the second is the component of the systematic uncertainty that is uncorrelated between bins, and the third is the correlated component.	Table_2.pdf [39 KiB] HiDef png [197 KiB] Thumbnail [109 KiB] tex code
Single differential production cross-sections (in $ {\rm \upmu b}$ ) for prompt $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu}$ mesons and $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu}$ from $b$ as functions of rapidity. The first uncertainty is statistical, the second is the component of the systematic uncertainty that is uncorrelated between bins, and the third is the correlated component.	Table_3.pdf [39 KiB] HiDef png [147 KiB] Thumbnail [79 KiB] tex code
Double differential production cross-sections (in ${\rm {\rm \upmu b} }/( {\mathrm{ Ge V /}c} )$) for prompt $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu}$ mesons and $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu}$ from $b$ as functions of $p_{\rm T}$ and $y$ in $ p\mathrm{Pb} $ forward data. The first uncertainty is statistical, the second is the component of the systematic uncertainty that is uncorrelated between bins, and the third is the correlated component.	Table_4.pdf [37 KiB] HiDef png [141 KiB] Thumbnail [46 KiB] tex code
Nuclear modification factor $R_{ p\mathrm{Pb} }$ as a function of $y$ with $ p_{\rm T} <14 {\mathrm{ Ge V /}c} $. The first uncertainty is statistical, the second is the systematic, and the third is the uncertainty related to the interpolation error.	Table_5.pdf [45 KiB] HiDef png [48 KiB] Thumbnail [23 KiB] tex code
Forward-backward production ratio $R_{ {FB}}$ as a function of $\|y\|$ with $ p_{\rm T} <14 {\mathrm{ Ge V /}c} $. The first uncertainty is statistical, the second is the uncorrelated systematic component, and the third is the systematic uncertainty correlated between bins.	Table_6.pdf [38 KiB] HiDef png [43 KiB] Thumbnail [18 KiB] tex code
Forward-backward production ratio $R_{ {FB}}$ as a function of $p_\mathrm{T}$ with $2.5<\|y\|<4.0$. The first uncertainty is statistical, the second is the uncorrelated systematic component, and the third is the systematic uncertainty correlated between bins.	Table_7.pdf [46 KiB] HiDef png [107 KiB] Thumbnail [46 KiB] tex code