AI summary · arXiv: 2301.05606v1 · nucl-ex

Measurement of suppression of large-radius jets and its dependence on substructure in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV with the ATLAS detector

ATLAS Collaboration

Original paper · DOI Submitted to arXiv on 13 Jan. 2023 Phys. Rev. Lett. 131, (2023) 172301 12 pages in total, no author list, 2 figures, 0 tables, submitted to Phys. Rev. Lett.. All figures including auxiliary figures are available at https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HION-2019-09/ License: CC BY 4.0

The essentials

  • ATLAS experiment conducted a measurement of nuclear modification factor of large-radius jets in Pb+Pb collisions at 5.02 TeV
  • Study focused on large-radius jets reconstructed using anti-$k_{t}$ algorithm with $R = 1.0$
  • Analysis done within kinematic range of $158 < p_{\mathrm{T}} < 1000$ GeV and $|y|<2.0$
  • Parameters like $\sqrt{d_{12}}$ and $\Delta R_{12}$ extracted to understand transverse momentum scale and angular separation within the jets
  • Significant observation: difference in quenching between single sub-jet structures and complex substructures in large-radius jets
  • Research supports hypothesis that large-radius jets with hard internal splittings experience greater energy loss during quenching processes

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AI-generated keywords: ATLAS experiment

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, , , , The ATLAS experiment has conducted a comprehensive measurement of the nuclear modification factor of large-radius jets in Pb+Pb collisions at a center-of-mass energy of 5.02 TeV. Utilizing data from 1.72 nb$^{-1}$ of Pb+Pb collisions and 257 pb$^{-1}$ of $pp$ collisions, the study focuses on large-radius jets reconstructed using the anti-$k_{t}$ algorithm with a radius parameter of $R = 1.0$. These jets are formed by re-clustering anti-$k_{t}$ $R = 0.2$ jets and are analyzed within the kinematic range of $158 < p_{\mathrm{T}} < 1000$ GeV and $|y|<2.0$. The constituents within these large-radius jets are further re-clustered using the $k_{t}$ algorithm to extract splitting parameters such as $\sqrt{d_{12}}$ and $\Delta R_{12}$. These parameters provide information on the transverse momentum scale and angular separation for the hardest splitting within each jet. The nuclear modification factor, denoted as $R_{\mathrm{AA}}$, is calculated by comparing jet yields in Pb+Pb collisions to those in $pp$ collisions as a function of jet transverse momentum ($p_{\mathrm{T}}$) and either $\sqrt{d_{12}}$ or $\Delta R_{12}$. One significant observation from this study is the distinct difference in quenching between large-radius jets with single sub-jet structures compared to those exhibiting more complex substructures. The analysis also includes a systematic comparison of jet suppression based on different jet definitions, shedding light on how various internal structures impact energy loss through quenching. Overall, the results presented in this study support the hypothesis that large-radius jets with hard internal splittings experience greater energy loss during quenching processes. This research provides valuable insights into understanding how jet structure influences jet suppression mechanisms in high-energy nuclear collisions, offering a new perspective on the role of internal substructure in determining energy loss patterns within these high-energy particle interactions.

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