Abstract <p>The authors present recent PHENIX measurements of the production of identified charged hadrons (<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11954_2025_5692_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\pi }^{ \pm }}\)</EquationSource> <!--BullPhys2571209Larionova-m1--> </InlineEquation>, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11954_2025_5692_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\({{K}^{ \pm }}\)</EquationSource> <!--BullPhys2571209Larionova-m2--> </InlineEquation>, <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11954_2025_5692_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(p\)</EquationSource> <!--BullPhys2571209Larionova-m3--> </InlineEquation>, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11954_2025_5692_Article_IEq4.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\bar {p}\)</EquationSource> <!--BullPhys2571209Larionova-m4--> </InlineEquation>) in <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11954_2025_5692_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(p\)</EquationSource> <!--BullPhys2571209Larionova-m5--> </InlineEquation> + Al, <sup>3</sup>He + Au, and Cu + Au collisions at <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11954_2025_5692_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="50" /> </InlineMediaObject> <EquationSource Format="TEX">\(\sqrt {{{s}_{{NN}}}} \)</EquationSource> <!--BullPhys2571209Larionova-m6--> </InlineEquation> = 200 GeV and in U + U collisions at <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11954_2025_5692_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="50" /> </InlineMediaObject> <EquationSource Format="TEX">\(\sqrt {{{s}_{{NN}}}} \)</EquationSource> <!--BullPhys2571209Larionova-m7--> </InlineEquation> = 193 GeV. The measured ratios of <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11954_2025_5692_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="44" /> </InlineMediaObject> <EquationSource Format="TEX">\(p{\text{/}}~{{\pi }^{ + }}\)</EquationSource> <!--BullPhys2571209Larionova-m8--> </InlineEquation> and <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11954_2025_5692_Article_IEq9.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="TEX">\(\bar {p}{\text{/}}{{\pi }^{ - }}\)</EquationSource> <!--BullPhys2571209Larionova-m9--> </InlineEquation> yields are compared to predictions made with the AMPT (string melting version) and PYTHIA/ANGANTYR program packages. Integral ratios of <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11954_2025_5692_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="44" /> </InlineMediaObject> <EquationSource Format="TEX">\(p{\text{/}}~{{\pi }^{ + }}\)</EquationSource> <!--BullPhys2571209Larionova-m10--> </InlineEquation>, <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11954_2025_5692_Article_IEq9.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="TEX">\(\bar {p}{\text{/}}{{\pi }^{ - }}\)</EquationSource> <!--BullPhys2571209Larionova-m11--> </InlineEquation>, <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11954_2025_5692_Article_IEq12.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\({{K}^{ + }}{\text{/}}{{\pi }^{ + }}\)</EquationSource> <!--BullPhys2571209Larionova-m12--> </InlineEquation>, <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11954_2025_5692_Article_IEq13.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\({{K}^{ - }}{\text{/}}{{\pi }^{ - }}\)</EquationSource> <!--BullPhys2571209Larionova-m13--> </InlineEquation> yields are presented as functions of the number of nucleons participating in nucleus–nucleus interactions.</p>

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Studying the Production of Identified Charged Hadrons in the PHENIX Experiment

  • D. M. Larionova,
  • Ya. A. Berdnikov,
  • D. O. Kotov

摘要

Abstract

The authors present recent PHENIX measurements of the production of identified charged hadrons ( \({{\pi }^{ \pm }}\) , \({{K}^{ \pm }}\) , \(p\) , \(\bar {p}\) ) in \(p\) + Al, 3He + Au, and Cu + Au collisions at \(\sqrt {{{s}_{{NN}}}} \) = 200 GeV and in U + U collisions at \(\sqrt {{{s}_{{NN}}}} \) = 193 GeV. The measured ratios of \(p{\text{/}}~{{\pi }^{ + }}\) and \(\bar {p}{\text{/}}{{\pi }^{ - }}\) yields are compared to predictions made with the AMPT (string melting version) and PYTHIA/ANGANTYR program packages. Integral ratios of \(p{\text{/}}~{{\pi }^{ + }}\) , \(\bar {p}{\text{/}}{{\pi }^{ - }}\) , \({{K}^{ + }}{\text{/}}{{\pi }^{ + }}\) , \({{K}^{ - }}{\text{/}}{{\pi }^{ - }}\) yields are presented as functions of the number of nucleons participating in nucleus–nucleus interactions.