<p>We present a comprehensive study of jet substructure observables in pp and PbPb collisions at <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\sqrt{s_\text {NN}} = 5.02\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msqrt> <msub> <mi>s</mi> <mtext>NN</mtext> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </mrow> </math></EquationSource> </InlineEquation>&#xa0;TeV using a multi-phase transport model. To suppress background contamination, the constituent subtraction method was employed for both PbPb and smeared pp events. The jet splitting momentum fraction (<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(z_\text {g}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>z</mi> <mtext>g</mtext> </msub> </math></EquationSource> </InlineEquation>) and the ratio of the groomed jet mass to the ungroomed jet transverse momentum (<InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(M_\text {g} / p_{\text {T},\text {jet}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>M</mi> <mtext>g</mtext> </msub> <mo stretchy="false">/</mo> <msub> <mi>p</mi> <mrow> <mtext>T</mtext> <mo>,</mo> <mtext>jet</mtext> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation>) were reconstructed using the Soft Drop algorithm with two grooming parameter settings. With <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(z_\text {cut} = 0.1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>z</mi> <mtext>cut</mtext> </msub> <mo>=</mo> <mn>0.1</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\beta = 0.0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>β</mi> <mo>=</mo> <mn>0.0</mn> </mrow> </math></EquationSource> </InlineEquation>, a slight modification in the <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(z_\text {g}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>z</mi> <mtext>g</mtext> </msub> </math></EquationSource> </InlineEquation> distribution is observed in central PbPb collisions, whereas a pronounced enhancement in the high <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(M_\text {g} / p_{\text {T},\text {jet}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>M</mi> <mtext>g</mtext> </msub> <mo stretchy="false">/</mo> <msub> <mi>p</mi> <mrow> <mtext>T</mtext> <mo>,</mo> <mtext>jet</mtext> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> region is found, particularly at low <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(p_{\text {T},\text {jet}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>p</mi> <mrow> <mtext>T</mtext> <mo>,</mo> <mtext>jet</mtext> </mrow> </msub> </math></EquationSource> </InlineEquation> and in more central events. A detailed analysis of the dynamical evolution stages revealed that this enhancement primarily originates from jet–medium interactions, whereas the contributions from hadronization and hadronic rescatterings are largely mitigated by the grooming procedure. In contrast, under a stronger grooming condition (<InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(z_\text {cut} = 0.5\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>z</mi> <mtext>cut</mtext> </msub> <mo>=</mo> <mn>0.5</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\beta = 1.5\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>β</mi> <mo>=</mo> <mn>1.5</mn> </mrow> </math></EquationSource> </InlineEquation>), no significant changes in <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(M_\text {g}/p_{\text {T},\text {jet}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>M</mi> <mtext>g</mtext> </msub> <mo stretchy="false">/</mo> <msub> <mi>p</mi> <mrow> <mtext>T</mtext> <mo>,</mo> <mtext>jet</mtext> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> are observed, indicating that the medium-induced modifications are predominantly associated with large-angle scattering within the AMPT framework.</p>

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Probing jet-medium interactions via jet substructure observables in relativistic heavy-ion collisions

  • Xiang-Pan Duan,
  • Tan Luo,
  • Guo-Liang Ma

摘要

We present a comprehensive study of jet substructure observables in pp and PbPb collisions at \(\sqrt{s_\text {NN}} = 5.02\) s NN = 5.02  TeV using a multi-phase transport model. To suppress background contamination, the constituent subtraction method was employed for both PbPb and smeared pp events. The jet splitting momentum fraction ( \(z_\text {g}\) z g ) and the ratio of the groomed jet mass to the ungroomed jet transverse momentum ( \(M_\text {g} / p_{\text {T},\text {jet}}\) M g / p T , jet ) were reconstructed using the Soft Drop algorithm with two grooming parameter settings. With \(z_\text {cut} = 0.1\) z cut = 0.1 and \(\beta = 0.0\) β = 0.0 , a slight modification in the \(z_\text {g}\) z g distribution is observed in central PbPb collisions, whereas a pronounced enhancement in the high \(M_\text {g} / p_{\text {T},\text {jet}}\) M g / p T , jet region is found, particularly at low \(p_{\text {T},\text {jet}}\) p T , jet and in more central events. A detailed analysis of the dynamical evolution stages revealed that this enhancement primarily originates from jet–medium interactions, whereas the contributions from hadronization and hadronic rescatterings are largely mitigated by the grooming procedure. In contrast, under a stronger grooming condition ( \(z_\text {cut} = 0.5\) z cut = 0.5 , \(\beta = 1.5\) β = 1.5 ), no significant changes in \(M_\text {g}/p_{\text {T},\text {jet}}\) M g / p T , jet are observed, indicating that the medium-induced modifications are predominantly associated with large-angle scattering within the AMPT framework.