This article presents measurements of the groomed jet radius and momen- tum splitting fraction in pp collisions at √s = 5.02 TeV with the ALICE detector at the Large Hadron Collider. Inclusive charged-particle jets are reconstructed at midrapidity using the anti-kT algorithm for transverse momentum 60 < pch jet T < 80 GeV/c. We report results using two different grooming algorithms: soft drop and, for the first time, dynam- ical grooming. For each grooming algorithm, a variety of grooming settings are used in order to explore the impact of collinear radiation on these jet substructure observables. These results are compared to perturbative calculations that include resummation of large logarithms at all orders in the strong coupling constant. We find good agreement of the theoretical predictions with the data for all grooming settings considered.

Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $$ \sqrt{s} $$ = 5.02 TeV

P. Cortese;L. Ramello;M. Sitta;
2023-01-01

Abstract

This article presents measurements of the groomed jet radius and momen- tum splitting fraction in pp collisions at √s = 5.02 TeV with the ALICE detector at the Large Hadron Collider. Inclusive charged-particle jets are reconstructed at midrapidity using the anti-kT algorithm for transverse momentum 60 < pch jet T < 80 GeV/c. We report results using two different grooming algorithms: soft drop and, for the first time, dynam- ical grooming. For each grooming algorithm, a variety of grooming settings are used in order to explore the impact of collinear radiation on these jet substructure observables. These results are compared to perturbative calculations that include resummation of large logarithms at all orders in the strong coupling constant. We find good agreement of the theoretical predictions with the data for all grooming settings considered.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11579/159003
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