Centrality and rapidity dependence of inclusive jet production in $\sqrt{s_\mathrm{NN}}$=5.02 TeV proton$-$lead collisions with the ATLAS detector

Measurements of the centrality and rapidity dependence of inclusive jet production in $\sqrt{s_\mathrm{NN}} = 5.02$ TeV proton--lead ($p$+Pb) collisions and the jet cross-section in $\sqrt{s} = 2.76$ TeV proton--proton collisions are presented. These quantities are measured in datasets corresponding to an integrated luminosity of 27.8 nb$^{-1}$ and 4.0 pb$^{-1}$, respectively, recorded with the ATLAS detector at the Large Hadron Collider in 2013. The $p$+Pb collision centrality was characterised using the total transverse energy measured in the pseudorapidity interval $-4.9 < \eta < -3.2$ in the direction of the lead beam. Results are presented for the double-differential per-collision yields as a function of jet rapidity and transverse momentum ($p_\mathrm{T}$) for minimum-bias and centrality-selected $p$+Pb collisions, and are compared to the jet rate from the geometric expectation. The total jet yield in minimum-bias events is slightly enhanced above the expectation in a $p_\mathrm{T}$-dependent manner but is consistent with the expectation within uncertainties. The ratios of jet spectra from different centrality selections show a strong modification of jet production at all $p_\mathrm{T}$ at forward rapidities and for large $p_\mathrm{T}$ at mid-rapidity, which manifests as a suppression of the jet yield in central events and an enhancement in peripheral events. These effects imply that the factorisation between hard and soft processes is violated at an unexpected level in proton--nucleus collisions. Furthermore, the modifications at forward rapidities are found to be a function of the total jet energy only, implying that the violations may have a simple dependence on the hard parton--parton kinematics.

12 December 2014

Contact: Heavy Ion Physics conveners internal

Figures

Figure 01


Distribution of ΣETPb for minimum-bias p+Pb collisions recorded during the 2013 run, measured in the FCal at -4.9 < η < -3.2 in the Pb-going direction. The vertical divisions correspond to the six centrality intervals used in this analysis. From right to left, the regions correspond to centrality intervals of 0–10%, 10–20%, 20–30%, 30–40%, 40–60% and 60–90%.

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Figure 02


Inclusive double-differential per-event jet yield in 0–90% p+Pb collisions as a function of jet pT in different y* bins. The yields are corrected for all detector effects. Vertical error bars represent the statistical uncertainty while the boxes represent the systematic uncertainties.

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Figure 03


Measured RpPb values for R=0.4 jets in 0–90% p+Pb collisions. Each panel shows the jet RpPb in a different rapidity range. Vertical error bars represent the statistical uncertainty while the boxes represent the systematic uncertainties on the jet yields. The shaded box at the left edge of the RpPb = 1 horizontal line indicates the systematic uncertainty on TpA and the mboxpp luminosity in quadrature. The shaded band represents a calculation using the EPS09 nuclear parton distribution function set.

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Figure 04


Centrality-dependent inclusive double-differential per-event jet yield in p+Pb collisions, for three different rapidity ranges. Each panel shows the yield in central (stars), mid-central (diamonds) and peripheral (crosses) events. The yields are corrected for all detector effects. Vertical error bars represent the statistical uncertainty while the boxes represent the systematic uncertainties.

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Figure 05


Measured RCP values for R=0.4 jets in p+Pb collisions in central (stars), mid-central (diamonds) and mid-peripheral (crosses) events. Each panel shows the jet RCP in a different rapidity range. Vertical error bars represent the statistical uncertainty while the boxes represent the systematic uncertainties on the jet yields. The shaded boxes at the left edge of the RCP = 1 horizontal line indicate the systematic uncertainty on Rcoll for (from left to right) peripheral, mid-central and central events.

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Figure 06


Measured RpPb values for R=0.4 jets in p+Pb collisions in central (stars), mid-central (diamonds) and peripheral (crosses) events. Each panel shows the jet RpPb in a different rapidity range. Vertical error bars represent the statistical uncertainty while the boxes represent the systematic uncertainties on the jet yields. The shaded boxes at the right edge of the RpPb = 1 horizontal line indicate the systematic uncertainties on TpA and the mboxpp luminosity added in quadrature for (from left to right) peripheral, mid-central and central events.

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Figure 07


Measured RCP values for R=0.4 jets in 0–10% p+Pb collisions. The panel on the left shows the five rapidity ranges that are the most forward-going, while the panel on the right shows the remaining five. The RCP values at each rapidity are plotted as a function of pT×cosh(<y*>), where <y*> is the midpoint of the rapidity bin. Vertical error bars represent the statistical uncertainty while the boxes represent the systematic uncertainties on the jet yields. The shaded box at the left edge (in the left panel) and right edge (in the right panel) of the RCP = 1 horizontal line indicates the systematic uncertainty on Rcoll.

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Figure 08


Measured RpPb values for R=0.4 jets in p+Pb collisions displayed for multiple rapidity ranges, showing 0–10% events in the left panel and 60–90% events in the right panel. The RpPb at each rapidity is plotted as a function of pT×cosh(<y*>), where <y*> is the midpoint of the rapidity bin. Vertical error bars represent the statistical uncertainty while the boxes represent the systematic uncertainties on the jet yields. The shaded box at the left edge of the RpPb = 1 horizontal line indicates the systematic uncertainties on TpA and the pp luminosity added in quadrature.

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Tables

Table 01


Average Rcoll and TpA values for the centrality intervals used in this analysis along with total systematic uncertainties. The Rcoll values are with respect to 60–90% events, where <Ncoll> = 2.98+0.21-0.29.

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