A. M. Khan, M. U. Ashraf, H. M. Alfanda, M. Uzair Aslam
{"title":"Dynamics of identified particles production in oxygen–oxygen collisions at \\(\\sqrt{s_{\\textrm{NN}}}=7\\) TeV using EPOS4","authors":"A. M. Khan, M. U. Ashraf, H. M. Alfanda, M. Uzair Aslam","doi":"10.1140/epja/s10050-024-01419-y","DOIUrl":null,"url":null,"abstract":"<div><p>The Large Hadron Collider (LHC) aims to inject oxygen (<sup>16</sup><i>O</i>) ions in the next run into its experiments. This include the anticipated one-day physics run focusing on <span>\\({O+O}\\,\\)</span>collisions at center-of-mass energy <span>\\(\\sqrt{s_{\\textrm{NN}}}=7\\)</span> TeV . In this study, we have used recently developed version of the EPOS (EPOS4) to study the production of identified particles (<span>\\(\\pi ^\\pm \\)</span>, <span>\\(K^\\pm \\)</span> and <span>\\(p({\\overline{p}})\\)</span>) in <span>\\({O+O}\\,\\)</span>collisions at <span>\\(\\sqrt{s_{\\textrm{NN}}}=7\\)</span> TeV . Predictions of transverse momentum (<span>\\({p_{\\textrm{T}}}\\,\\)</span>) spectra, <span>\\({\\langle p_{\\textrm{T}} \\rangle }\\,\\)</span>, integrated yield (<span>\\({{\\mathrm d}N{/}{\\mathrm d}{\\textit{y}}}\\,\\)</span>) for different centrality classes are studied. To provide insight into the collective nature of the produced particles, we look into the <span>\\({p_{\\textrm{T}}}\\,\\)</span>-differential particle ratios (<span>\\(K/\\pi \\)</span> and <span>\\(p/\\pi \\)</span>) and <span>\\({p_{\\textrm{T}}}\\,\\)</span>-integrated particle ratios to (<span>\\(\\pi ^++\\pi ^-\\)</span>) as a function of charge particle multiplicity. The shape of the charge particle multiplicity (<span>\\({\\textrm{d}N_\\textrm{ch}/\\textrm{d}\\eta }\\,\\)</span>) and mean transverse momentum (<span>\\({\\langle p_{\\textrm{T}} \\rangle }\\,\\)</span>) is well described by EPOS4. The predictions for the ratios of <span>\\(K/\\pi \\)</span> and <span>\\(p/\\pi \\)</span> from EPOS4 exhibit a systematic overestimation compared to the trends observed in <span>\\({p+p}\\,\\)</span>, <span>\\({p+Pb}\\,\\)</span>and <span>\\({Pb+Pb}\\,\\)</span>systems as a function of charged-particle multiplicity. Interestingly, the <span>\\({O+O}\\,\\)</span>results of <span>\\({p_{\\textrm{T}}}\\,\\)</span>-integrated particle ratios shows a clear final state multiplicity overlap with <span>\\({p+p}\\,\\)</span>, <span>\\({p+Pb}\\,\\)</span>and <span>\\({Pb+Pb}\\,\\)</span>collisions. EPOS4 does not only mimics signs of collectivity, but embeds collective expansion by construction, since it relies on relativistic hydrodynamics to model the evolution of the so-called core and is one of the suitable candidates to study ultra-relativistic heavy-ion collisions. Furthermore, the foreseen data from <span>\\({O+O}\\,\\)</span>collisions at the LHC, when available, will help to better understand the heavy-ion-like behavior in small systems as well as help to put possible constraints on the model parameters.</p></div>","PeriodicalId":786,"journal":{"name":"The European Physical Journal A","volume":"60 10","pages":""},"PeriodicalIF":2.6000,"publicationDate":"2024-10-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"The European Physical Journal A","FirstCategoryId":"4","ListUrlMain":"https://link.springer.com/article/10.1140/epja/s10050-024-01419-y","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, NUCLEAR","Score":null,"Total":0}
引用次数: 0
Abstract
The Large Hadron Collider (LHC) aims to inject oxygen (16O) ions in the next run into its experiments. This include the anticipated one-day physics run focusing on \({O+O}\,\)collisions at center-of-mass energy \(\sqrt{s_{\textrm{NN}}}=7\) TeV . In this study, we have used recently developed version of the EPOS (EPOS4) to study the production of identified particles (\(\pi ^\pm \), \(K^\pm \) and \(p({\overline{p}})\)) in \({O+O}\,\)collisions at \(\sqrt{s_{\textrm{NN}}}=7\) TeV . Predictions of transverse momentum (\({p_{\textrm{T}}}\,\)) spectra, \({\langle p_{\textrm{T}} \rangle }\,\), integrated yield (\({{\mathrm d}N{/}{\mathrm d}{\textit{y}}}\,\)) for different centrality classes are studied. To provide insight into the collective nature of the produced particles, we look into the \({p_{\textrm{T}}}\,\)-differential particle ratios (\(K/\pi \) and \(p/\pi \)) and \({p_{\textrm{T}}}\,\)-integrated particle ratios to (\(\pi ^++\pi ^-\)) as a function of charge particle multiplicity. The shape of the charge particle multiplicity (\({\textrm{d}N_\textrm{ch}/\textrm{d}\eta }\,\)) and mean transverse momentum (\({\langle p_{\textrm{T}} \rangle }\,\)) is well described by EPOS4. The predictions for the ratios of \(K/\pi \) and \(p/\pi \) from EPOS4 exhibit a systematic overestimation compared to the trends observed in \({p+p}\,\), \({p+Pb}\,\)and \({Pb+Pb}\,\)systems as a function of charged-particle multiplicity. Interestingly, the \({O+O}\,\)results of \({p_{\textrm{T}}}\,\)-integrated particle ratios shows a clear final state multiplicity overlap with \({p+p}\,\), \({p+Pb}\,\)and \({Pb+Pb}\,\)collisions. EPOS4 does not only mimics signs of collectivity, but embeds collective expansion by construction, since it relies on relativistic hydrodynamics to model the evolution of the so-called core and is one of the suitable candidates to study ultra-relativistic heavy-ion collisions. Furthermore, the foreseen data from \({O+O}\,\)collisions at the LHC, when available, will help to better understand the heavy-ion-like behavior in small systems as well as help to put possible constraints on the model parameters.
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