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Measurement of the inclusive differential jet cross section in pp collisions at $\sqrt{s}$ = 2.76 TeV

ALICE Collaboration

TL;DR

This paper reports the first measurement of the inclusive differential jet cross section at mid-rapidity in pp collisions at $\sqrt{s}=2.76$ TeV with the ALICE detector, providing a crucial reference for heavy-ion jet studies and a test of pQCD. Jets are reconstructed with the anti-$k_T$ algorithm for radii $R=0.2$ and $R=0.4$ and corrected to the particle level, with careful treatment of trigger biases and underlying-event contributions. The results are compared to Next-to-Leading Order pQCD calculations, showing good agreement when hadronization is included, and the cross-section ratio between the two radii offers insight into jet substructure and radiation patterns. This measurement, also consistent with prior 7 TeV data, strengthens the empirical foundation for jet physics at LHC energies and informs future jet-quenching studies in heavy-ion collisions at the same energy.

Abstract

The ALICE collaboration at the CERN Large Hadron Collider reports the first measurement of the inclusive differential jet cross section at mid-rapidity in pp collisions at $\sqrt{s} = 2.76$ TeV, with integrated luminosity of 13.6 nb$^{-1}$. Jets are measured over the transverse momentum range 20 to 125 GeV/c and are corrected to the particle level. Calculations based on Next-to-Leading Order perturbative QCD are in good agreement with the measurements. The ratio of inclusive jet cross sections for jet radii $R = 0.2$ and $R = 0.4$ is reported, and is also well reproduced by a Next-to-Leading Order perturbative QCD calculation when hadronization effects are included.

Measurement of the inclusive differential jet cross section in pp collisions at $\sqrt{s}$ = 2.76 TeV

TL;DR

This paper reports the first measurement of the inclusive differential jet cross section at mid-rapidity in pp collisions at TeV with the ALICE detector, providing a crucial reference for heavy-ion jet studies and a test of pQCD. Jets are reconstructed with the anti- algorithm for radii and and corrected to the particle level, with careful treatment of trigger biases and underlying-event contributions. The results are compared to Next-to-Leading Order pQCD calculations, showing good agreement when hadronization is included, and the cross-section ratio between the two radii offers insight into jet substructure and radiation patterns. This measurement, also consistent with prior 7 TeV data, strengthens the empirical foundation for jet physics at LHC energies and informs future jet-quenching studies in heavy-ion collisions at the same energy.

Abstract

The ALICE collaboration at the CERN Large Hadron Collider reports the first measurement of the inclusive differential jet cross section at mid-rapidity in pp collisions at TeV, with integrated luminosity of 13.6 nb. Jets are measured over the transverse momentum range 20 to 125 GeV/c and are corrected to the particle level. Calculations based on Next-to-Leading Order perturbative QCD are in good agreement with the measurements. The ratio of inclusive jet cross sections for jet radii and is reported, and is also well reproduced by a Next-to-Leading Order perturbative QCD calculation when hadronization effects are included.

Paper Structure

This paper contains 7 sections, 1 equation, 4 figures, 2 tables.

Figures (4)

  • Figure 1: Jet neutral energy fraction (NEF) distributions for MB data (open squares), EMCal-triggered data (filled circles) and simulations (histograms), in four different $p_{\mathrm{T,jet}}$ intervals.
  • Figure 2: Simulated detector response to jets. Upper panels: probability distribution of $\left(p_\mathrm{T,jet}^\mathrm{detector}-p_\mathrm{T,jet}^\mathrm{particle}\right)/p_\mathrm{T,jet}^\mathrm{particle}$, in intervals of $p_\mathrm{T,jet}^\mathrm{particle}$. Lower left: mean and median of distribution as a function of $p_\mathrm{T,jet}^\mathrm{particle}$. Lower right: standard deviation of distribution as a function of $p_\mathrm{T,jet}^\mathrm{particle}$. The statistical errors are smaller than the marker size.
  • Figure 3: Upper panels: inclusive differential jet cross sections for $R$ = 0.2 (left) and $R$ = 0.4 (right). Vertical bars show the statistical error, while boxes show the systematic uncertainty (Table \ref{['tab:Table2']}). The bands show the NLO pQCD calculations discussed in the text ArmestoSoyez:2011np. Lower panels: ratio of NLO pQCD calculations to data. Data points are placed at the center of each bin.
  • Figure 4: Ratio of inclusive differential jet cross sections for $R$ = 0.2 and $R$ = 0.4, with pQCD calculations from Soyez:2011np. Data points are placed at the center of each bin.