<p>This work compares identified-hadron <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(p_T\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>p</mi> <mi>T</mi> </msub> </math></EquationSource> </InlineEquation> spectra in Au+Au collisions at <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\sqrt{s}=7.7\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>7.7</mn> </mrow> </math></EquationSource> </InlineEquation>&#xa0;GeV, measured by the STAR experiment at RHIC, with results from common event generators. We use EPOS (EPOSLHC and EPOS4) and Pythia8 and confront them directly with the data. The study covers <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\pi ^\pm \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>π</mi> <mo>±</mo> </msup> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(K^\pm \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>K</mi> <mo>±</mo> </msup> </math></EquationSource> </InlineEquation>, and protons-antiprotons at mid-rapidity (<InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(|y|&lt;0.1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">|</mo> <mi>y</mi> <mo stretchy="false">|</mo> <mo>&lt;</mo> <mn>0.1</mn> </mrow> </math></EquationSource> </InlineEquation>) in nine centrality bins.</p><p>Pythia8 tends to overestimate pion data and misrepresents kaons and (anti-)protons depending on centrality. EPOS4 described the pions spectra well in comparison with Pythia8 consistent with the inclusion of hadronic re-scattering in the model. EPOSLHC aligns with experimental data better at higher <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(p_T\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>p</mi> <mi>T</mi> </msub> </math></EquationSource> </InlineEquation> for pions and anti-protons but underestimates kaons and protons in most centrality bins. At larger <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(p_T\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>p</mi> <mi>T</mi> </msub> </math></EquationSource> </InlineEquation>, suppression is observed in EPOSLHC tune which may reflect the collective flow that affects high <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(p_T\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>p</mi> <mi>T</mi> </msub> </math></EquationSource> </InlineEquation> particles. The EPOS4 model generally matches data well across centrality bins for <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\pi ^\pm \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>π</mi> <mo>±</mo> </msup> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(K^\pm \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>K</mi> <mo>±</mo> </msup> </math></EquationSource> </InlineEquation> mesons, and anti-protons, but its accuracy diminishes in peripheral collisions, particularly underestimating protons at high <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(p_T\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>p</mi> <mi>T</mi> </msub> </math></EquationSource> </InlineEquation> consistent with weaker final-state interaction effects in smaller systems. Additionally, suppression is observed in EPOS4 in protons and anti-protons, which may be influenced by baryon–anti-baryon annihilation channels implemented in the model. In general, EPOS4 and EPOSLHC provide a closer description than Pythia8 in the measured range, consistent with their inclusion of collective dynamics and hadronic re-scattering. Additionally, the extracted freeze-out parameters show that effective temperature rises and the non-extensive parameter decreases with increasing centrality, indicating greater system excitation and faster thermal equilibration in central collisions.</p>

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The Phenomenological Models Prediction to Study the \(p_T\) Spectra of Identified Hadrons in Au+Au Collisions at \(\sqrt{s}=7.7\) GeV

  • Maryam Waqar,
  • Haifa I. Alrebdi,
  • Muhammad Ajaz,
  • Muhammad Waqas,
  • Mohammad Ayaz Ahmad,
  • Refka Ghodhbani

摘要

This work compares identified-hadron \(p_T\) p T spectra in Au+Au collisions at \(\sqrt{s}=7.7\) s = 7.7  GeV, measured by the STAR experiment at RHIC, with results from common event generators. We use EPOS (EPOSLHC and EPOS4) and Pythia8 and confront them directly with the data. The study covers \(\pi ^\pm \) π ± , \(K^\pm \) K ± , and protons-antiprotons at mid-rapidity ( \(|y|<0.1\) | y | < 0.1 ) in nine centrality bins.

Pythia8 tends to overestimate pion data and misrepresents kaons and (anti-)protons depending on centrality. EPOS4 described the pions spectra well in comparison with Pythia8 consistent with the inclusion of hadronic re-scattering in the model. EPOSLHC aligns with experimental data better at higher \(p_T\) p T for pions and anti-protons but underestimates kaons and protons in most centrality bins. At larger \(p_T\) p T , suppression is observed in EPOSLHC tune which may reflect the collective flow that affects high \(p_T\) p T particles. The EPOS4 model generally matches data well across centrality bins for \(\pi ^\pm \) π ± , \(K^\pm \) K ± mesons, and anti-protons, but its accuracy diminishes in peripheral collisions, particularly underestimating protons at high \(p_T\) p T consistent with weaker final-state interaction effects in smaller systems. Additionally, suppression is observed in EPOS4 in protons and anti-protons, which may be influenced by baryon–anti-baryon annihilation channels implemented in the model. In general, EPOS4 and EPOSLHC provide a closer description than Pythia8 in the measured range, consistent with their inclusion of collective dynamics and hadronic re-scattering. Additionally, the extracted freeze-out parameters show that effective temperature rises and the non-extensive parameter decreases with increasing centrality, indicating greater system excitation and faster thermal equilibration in central collisions.