Production of leptons from decay of heavy-flavor hadrons in high-energy nuclear collisions

This paper presents a theoretical study on the production of leptons from decay of heavy-flavor hadrons (denoted as HFLs) in high-energy nuclear collisions at the CERN Large Hadron Collider. The <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mi mathvariant="italic">pp</a:mi></a:math> baseline is calculated by the fonll program, which matches the next-to-leading order perturbative QCD (pQCD) calculation with the next-to-leading-logarithm large-<c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:msub><c:mi>p</c:mi><c:mi>T</c:mi></c:msub></c:math> resummation. The in-medium propagation of heavy quarks is driven by the modified Langevin equations, which consider both the elastic and inelastic partonic interactions. We propose a method to separate the respective influence of the six factors, i.e., <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"><d:mi mathvariant="italic">pp</d:mi></d:math> spectra, cold nuclear matter (CNM) effects, in-medium energy loss (E-loss), fragmentation functions (FFs), coalescence (Coal), and decay channels, which may contribute to the larger <f:math xmlns:f="http://www.w3.org/1998/Math/MathML"><f:msub><f:mi>R</f:mi><f:mrow><f:mi>A</f:mi><f:mi>A</f:mi></f:mrow></f:msub></f:math> of HFL <g:math xmlns:g="http://www.w3.org/1998/Math/MathML"><g:mrow><g:mo>←</g:mo><g:mi>b</g:mi></g:mrow></g:math> compared to that of HFL <h:math xmlns:h="http://www.w3.org/1998/Math/MathML"><h:mrow><h:mo>←</h:mo><h:mi>c</h:mi></h:mrow></h:math> in nucleus-nucleus collisions. Based on quantitative analysis, we demonstrate that both coalescence hadronization decay channels and the mass-dependent E-loss play an essential role at <i:math xmlns:i="http://www.w3.org/1998/Math/MathML"><i:mrow><i:msub><i:mi>p</i:mi><i:mi>T</i:mi></i:msub><i:mo>&lt;</i:mo><i:mn>5</i:mn><i:mspace width="0.16em"/><i:mi>GeV</i:mi></i:mrow></i:math>, while the latter dominates the higher <k:math xmlns:k="http://www.w3.org/1998/Math/MathML"><k:msub><k:mi>p</k:mi><k:mi>T</k:mi></k:msub></k:math> region. It is also found that the influences of the CNM effects and FFs are insignificant. At the same time, different initial <l:math xmlns:l="http://www.w3.org/1998/Math/MathML"><l:mi mathvariant="italic">pp</l:mi></l:math> spectra of charm and bottom quarks have a considerable impact at <n:math xmlns:n="http://www.w3.org/1998/Math/MathML"><n:mrow><n:msub><n:mi>p</n:mi><n:mi>T</n:mi></n:msub><n:mo>&gt;</n:mo><n:mn>5</n:mn><n:mspace width="0.16em"/><n:mi>GeV</n:mi></n:mrow></n:math>. Furthermore, we explore the path-length dependence of jet quenching by comparing the HFL <p:math xmlns:p="http://www.w3.org/1998/Math/MathML"><p:msub><p:mi>R</p:mi><p:mrow><p:mi>A</p:mi><p:mi>A</p:mi></p:mrow></p:msub></p:math> in two different collision systems. Our investigations show smaller HFL <q:math xmlns:q="http://www.w3.org/1998/Math/MathML"><q:msub><q:mi>R</q:mi><q:mrow><q:mi>A</q:mi><q:mi>A</q:mi></q:mrow></q:msub></q:math> in <r:math xmlns:r="http://www.w3.org/1998/Math/MathML"><r:mrow><r:mi>Pb</r:mi><r:mo>+</r:mo><r:mi>Pb</r:mi></r:mrow></r:math> than in <s:math xmlns:s="http://www.w3.org/1998/Math/MathML"><s:mrow><s:mi>Xe</s:mi><s:mo>+</s:mo><s:mi>Xe</s:mi></s:mrow></s:math> within the same centrality bin, consistent with the ALICE data. The longer propagation time and more effective energy loss of heavy quarks in <t:math xmlns:t="http://www.w3.org/1998/Math/MathML"><t:mrow><t:mi>Pb</t:mi><t:mo>+</t:mo><t:mi>Pb</t:mi></t:mrow></t:math> collisions play critical roles in the stronger yield suppression of the HFLs compared to that in <u:math xmlns:u="http://www.w3.org/1998/Math/MathML"><u:mrow><u:mi>Xe</u:mi><u:mo>+</u:mo><u:mi>Xe</u:mi></u:mrow></u:math>. In addition, we observe a scaling behavior of the HFL <v:math xmlns:v="http://www.w3.org/1998/Math/MathML"><v:msub><v:mi>R</v:mi><v:mrow><v:mi>A</v:mi><v:mi>A</v:mi></v:mrow></v:msub></v:math> in <w:math xmlns:w="http://www.w3.org/1998/Math/MathML"><w:mrow><w:mi>Xe</w:mi><w:mo>+</w:mo><w:mi>Xe</w:mi></w:mrow></w:math> and <x:math xmlns:x="http://www.w3.org/1998/Math/MathML"><x:mrow><x:mi>Pb</x:mi><x:mo>+</x:mo><x:mi>Pb</x:mi></x:mrow></x:math> collisions.

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Journal
Physical review. C
Published
2025-03-24
DOI
https://doi.org/10.1103/physrevc.111.034912
Primary Topic
High-Energy Particle Collisions Research
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article
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0.00

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article

Production of leptons from decay of heavy-flavor hadrons in high-energy nuclear collisions

Enke Wang, Sa Wang, Shuwan Shen, Yao Li et al.
Physical review. C
High-Energy Particle Collisions Research
article

Production of leptons from decay of heavy-flavor hadrons in high-energy nuclear collisions

Enke Wang, Sa Wang, Shuwan Shen, Yao Li, Ben-Wei Zhang
article en

Abstract

This paper presents a theoretical study on the production of leptons from decay of heavy-flavor hadrons (denoted as HFLs) in high-energy nuclear collisions at the CERN Large Hadron Collider. The <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mi mathvariant="italic">pp</a:mi></a:math> baseline is calculated by the fonll program, which matches the next-to-leading order perturbative QCD (pQCD) calculation with the next-to-leading-logarithm large-<c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:msub><c:mi>p</c:mi><c:mi>T</c:mi></c:msub></c:math> resummation. The in-medium propagation of heavy quarks is driven by the modified Langevin equations, which consider both the elastic and inelastic partonic interactions. We propose a method to separate the respective influence of the six factors, i.e., <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"><d:mi mathvariant="italic">pp</d:mi></d:math> spectra, cold nuclear matter (CNM) effects, in-medium energy loss (E-loss), fragmentation functions (FFs), coalescence (Coal), and decay channels, which may contribute to the larger <f:math xmlns:f="http://www.w3.org/1998/Math/MathML"><f:msub><f:mi>R</f:mi><f:mrow><f:mi>A</f:mi><f:mi>A</f:mi></f:mrow></f:msub></f:math> of HFL <g:math xmlns:g="http://www.w3.org/1998/Math/MathML"><g:mrow><g:mo>←</g:mo><g:mi>b</g:mi></g:mrow></g:math> compared to that of HFL <h:math xmlns:h="http://www.w3.org/1998/Math/MathML"><h:mrow><h:mo>←</h:mo><h:mi>c</h:mi></h:mrow></h:math> in nucleus-nucleus collisions. Based on quantitative analysis, we demonstrate that both coalescence hadronization decay channels and the mass-dependent E-loss play an essential role at <i:math xmlns:i="http://www.w3.org/1998/Math/MathML"><i:mrow><i:msub><i:mi>p</i:mi><i:mi>T</i:mi></i:msub><i:mo>&lt;</i:mo><i:mn>5</i:mn><i:mspace width="0.16em"/><i:mi>GeV</i:mi></i:mrow></i:math>, while the latter dominates the higher <k:math xmlns:k="http://www.w3.org/1998/Math/MathML"><k:msub><k:mi>p</k:mi><k:mi>T</k:mi></k:msub></k:math> region. It is also found that the influences of the CNM effects and FFs are insignificant. At the same time, different initial <l:math xmlns:l="http://www.w3.org/1998/Math/MathML"><l:mi mathvariant="italic">pp</l:mi></l:math> spectra of charm and bottom quarks have a considerable impact at <n:math xmlns:n="http://www.w3.org/1998/Math/MathML"><n:mrow><n:msub><n:mi>p</n:mi><n:mi>T</n:mi></n:msub><n:mo>&gt;</n:mo><n:mn>5</n:mn><n:mspace width="0.16em"/><n:mi>GeV</n:mi></n:mrow></n:math>. Furthermore, we explore the path-length dependence of jet quenching by comparing the HFL <p:math xmlns:p="http://www.w3.org/1998/Math/MathML"><p:msub><p:mi>R</p:mi><p:mrow><p:mi>A</p:mi><p:mi>A</p:mi></p:mrow></p:msub></p:math> in two different collision systems. Our investigations show smaller HFL <q:math xmlns:q="http://www.w3.org/1998/Math/MathML"><q:msub><q:mi>R</q:mi><q:mrow><q:mi>A</q:mi><q:mi>A</q:mi></q:mrow></q:msub></q:math> in <r:math xmlns:r="http://www.w3.org/1998/Math/MathML"><r:mrow><r:mi>Pb</r:mi><r:mo>+</r:mo><r:mi>Pb</r:mi></r:mrow></r:math> than in <s:math xmlns:s="http://www.w3.org/1998/Math/MathML"><s:mrow><s:mi>Xe</s:mi><s:mo>+</s:mo><s:mi>Xe</s:mi></s:mrow></s:math> within the same centrality bin, consistent with the ALICE data. The longer propagation time and more effective energy loss of heavy quarks in <t:math xmlns:t="http://www.w3.org/1998/Math/MathML"><t:mrow><t:mi>Pb</t:mi><t:mo>+</t:mo><t:mi>Pb</t:mi></t:mrow></t:math> collisions play critical roles in the stronger yield suppression of the HFLs compared to that in <u:math xmlns:u="http://www.w3.org/1998/Math/MathML"><u:mrow><u:mi>Xe</u:mi><u:mo>+</u:mo><u:mi>Xe</u:mi></u:mrow></u:math>. In addition, we observe a scaling behavior of the HFL <v:math xmlns:v="http://www.w3.org/1998/Math/MathML"><v:msub><v:mi>R</v:mi><v:mrow><v:mi>A</v:mi><v:mi>A</v:mi></v:mrow></v:msub></v:math> in <w:math xmlns:w="http://www.w3.org/1998/Math/MathML"><w:mrow><w:mi>Xe</w:mi><w:mo>+</w:mo><w:mi>Xe</w:mi></w:mrow></w:math> and <x:math xmlns:x="http://www.w3.org/1998/Math/MathML"><x:mrow><x:mi>Pb</x:mi><x:mo>+</x:mo><x:mi>Pb</x:mi></x:mrow></x:math> collisions.

Physical review. CVol. 111(3)
China Three Gorges University (CN), South China Normal University (CN), Central China Normal University (CN)
National Natural Science Foundation of China, China Postdoctoral Science Foundation, Key Laboratory of Quark and Lepton Physics
Openalex Percentile: Top 97%
High-Energy Particle Collisions Research
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