A. M. Khan, M. U. Ashraf, H. M. Alfanda, M. Uzair Aslam
{"title":"使用 EPOS4 在(\\sqrt{s_{textrm{NN}}}=7\\)TeV 的氧-氧对撞中识别粒子产生的动力学特性","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":"{\"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}","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}
Dynamics of identified particles production in oxygen–oxygen collisions at \(\sqrt{s_{\textrm{NN}}}=7\) TeV using EPOS4
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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