Szczegóły publikacji

Opis bibliograficzny

Measurement of substructure-dependent suppression of large-radius jets with charged particles in Pb+Pb collisions with ATLAS / G. Aad, [et al.], L. ADAMCZYK, [et al.], P. BALEK, [et al.], T. BOŁD, [et al.], K. M. CIEŚLA, [et al.], W. DĄBROWSKI, [et al.], K. DOMIJAN, [et al.], M. DYNDAŁ, [et al.], A. K. GILBERT, [et al.], I. GRABOWSKA-BOŁD, [et al.], S. KOPERNY, [et al.], K. MAJ, [et al.], B. MINDUR, [et al.], P. MOSZKOWICZ, [et al.], P. A. POTĘPA, [et al.], M. PRZYBYCIEŃ, [et al.], P. RYBCZYŃSKI, [et al.] // Physics Letters . B ; ISSN  0370-2693. — 2025 — vol. 871 art. no. 139929, s. 1–17. — Bibliogr. s. 16–17, Abstr. — Publikacja dostępna online od: 2025-11-07

Autorzy (2968)

Słowa kluczowe

jet quenchingrelativistic heavy ion collisionsquark-gluon plasmajetsheavy flavor physics

Dane bibliometryczne

ID BaDAP165040
Data dodania do BaDAP2025-12-19
Tekst źródłowyURL
DOI10.1016/j.physletb.2025.139929
Rok publikacji2025
Typ publikacjiartykuł w czasopiśmie
Otwarty dostęptak
Creative Commons
Czasopismo/seriaPhysics Letters, B

Abstract

Measurements of jet substructure in Pb+Pb collisions provide key insights into the mechanism of jet quenching in the hot and dense QCD medium created in these collisions.This Letter presents a measurement of the suppression of large-radius jets with a radius parameter of R = 1.0 and its dependence on the jet substructure. The measurement uses 1.72 nb-1 of Pb+Pb data and 255 pb−1 of pp data, both at √sNN = 5.02 TeV, recorded with the ATLAS detector at the Large Hadron Collider. Large-radius jets are reconstructed by reclustering R = 0.2 calorimetric jets and are measured for transverse momentum above 200 GeV. Jet substructure is evaluated using charged-particle tracks, and the overall level of jet suppression is quantified using the jet nuclear modification factor (RAA). The jet RAA is measured as a function of jet pT, the charged kt splitting scale (√d12), and the angular separation (ΔR12) of two leading sub-jets. The jet RAA gradually decreases with increasing √d12, implying significantly stronger suppression of large-radius jets with larger kt splitting scale. The jet RAA gradually decreases for ΔR12 in the range 0.01−0.2 and then remains consistent with a constant for ΔR12 ≳ 0.2. The observed significant dependence of jet suppression on the jet substructure will provide new insights into its role in the quenching process.

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