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Measurement of event shapes at large momentum transfer with the ATLAS detector in pp collisions at sqrt(s) = 7 TeV

ATLAS Collaboration

TL;DR

This ATLAS study measures six jet-based event shapes in 7 TeV pp collisions using 35 pb^-1 to probe multi-jet topologies and test LO Monte Carlo generators with leading-log parton showers. The observables are unfolded to particle level and analyzed as functions of the kinematic scale defined by $ rac{1}{2}H_{{ m T},2}$, revealing general agreement with Pythia and Alpgen predictions and highlighting areas where Herwig++ underperforms, especially for aplanarity. The results support the importance of leading-log resummation in MC models and provide data-driven input for tuning generators, with implications for precise QCD studies and background modeling in multi-jet final states. Overall, the HT2-dependence of the mean event-shape values mirrors the running of $oldsymbol{\\alpha_s}$ and demonstrates the capability of ATLAS jet-based event shapes to constrain QCD dynamics at high momentum transfers.

Abstract

A measurement of event shape variables is presented for large momentum transfer proton-proton collisions using the ATLAS detector at the Large Hadron Collider. Six event shape variables calculated using hadronic jets are studied in inclusive multi-jet events in 35 pb^-1 of integrated luminosity at a center-of-mass energy of sqrt(s) = 7 TeV. These measurements are compared to predictions by three Monte Carlo event generators containing leading-logarithmic parton showers matched to leading order matrix elements for 2 to 2 and 2 to n (n=2,...6) scattering. Measurements of the third-jet resolution parameter, aplanarity, thrust, sphericity, and transverse sphericity are generally well described. The mean value of each event shape variable is evaluated as a function of the average momentum of the two leading jets pT1 and pT2, with a mean pT approaching 1 TeV.

Measurement of event shapes at large momentum transfer with the ATLAS detector in pp collisions at sqrt(s) = 7 TeV

TL;DR

This ATLAS study measures six jet-based event shapes in 7 TeV pp collisions using 35 pb^-1 to probe multi-jet topologies and test LO Monte Carlo generators with leading-log parton showers. The observables are unfolded to particle level and analyzed as functions of the kinematic scale defined by , revealing general agreement with Pythia and Alpgen predictions and highlighting areas where Herwig++ underperforms, especially for aplanarity. The results support the importance of leading-log resummation in MC models and provide data-driven input for tuning generators, with implications for precise QCD studies and background modeling in multi-jet final states. Overall, the HT2-dependence of the mean event-shape values mirrors the running of and demonstrates the capability of ATLAS jet-based event shapes to constrain QCD dynamics at high momentum transfers.

Abstract

A measurement of event shape variables is presented for large momentum transfer proton-proton collisions using the ATLAS detector at the Large Hadron Collider. Six event shape variables calculated using hadronic jets are studied in inclusive multi-jet events in 35 pb^-1 of integrated luminosity at a center-of-mass energy of sqrt(s) = 7 TeV. These measurements are compared to predictions by three Monte Carlo event generators containing leading-logarithmic parton showers matched to leading order matrix elements for 2 to 2 and 2 to n (n=2,...6) scattering. Measurements of the third-jet resolution parameter, aplanarity, thrust, sphericity, and transverse sphericity are generally well described. The mean value of each event shape variable is evaluated as a function of the average momentum of the two leading jets pT1 and pT2, with a mean pT approaching 1 TeV.

Paper Structure

This paper contains 14 sections, 4 equations, 3 figures.

Figures (3)

  • Figure 1: Inclusive jet trigger efficiency as a function of $\frac{1}{2}H_{{\rm T},2}\xspace$ evaluated offline. The efficiency to select events with $\frac{1}{2}H_{{\rm T},2}\xspace\xspace > 250$ GeV using this trigger is greater than 99.8%.
  • Figure 2: Unfolded hadron-level distributions of the \ref{['fig:eventshapes:unfolded:lny23']} third-jet resolution parameter, $\ln y_{23}\xspace$, \ref{['fig:eventshapes:unfolded:apl']} aplanarity, $A$, \ref{['fig:eventshapes:unfolded:thrustMajor']} transverse thrust, $\tau_{\perp}$, \ref{['fig:eventshapes:unfolded:thrustMinor']} minor component of the transverse thrust, $T_{m,\perp}$, \ref{['fig:eventshapes:unfolded:sph']} sphericity, $S$, and \ref{['fig:eventshapes:unfolded:sphtranv']} transverse sphericity, $S_{\perp}$. The uncertainty shown for the data includes statistical and systematic uncertainties.
  • Figure 3: Mean value of each event shape variable as a function of $\frac{1}{2}H_{{\rm T},2}\xspace$. Comparisons are made between the MC generators Herwig++, Alpgen and Pythia.