{"title":"用PYTHIA 8.312模拟的p-Pb碰撞中作为 \"中心性 \"估计的平坦性 Angantyr","authors":"Antonio Ortiz, Gyula Bencedi, Feng Fan","doi":"arxiv-2407.07724","DOIUrl":null,"url":null,"abstract":"In this paper, a \"centrality\" estimator based on flattenicity ($\\rho$) is\nstudied in proton-led (p-Pb) collisions at $\\sqrt{s_{\\rm NN}}=5.02$ TeV using\nPYTHIA 8 Angantyr. Although Angantyr is still under development, the existing\nimplementation is enough to study the particle production in systems where\nmedium effects are absent. Firstly, ALICE data on pseudorapidity distributions\nas a function of the forward multiplicity (V0M), as well as transverse momentum\ndistributions of identified particles in non-single diffractive p-Pb\ncollisions, are compared with Angantyr. Secondly, the average number of binary\nnucleon-nucleon ($N_{\\rm coll}$) collisions for different \"centrality\"\nestimators are compared. The studies include the following \"centrality\"\nestimators: V0M, $\\rho$ and midrapidity multiplicity (CL1). On one hand, the\n\"centrality\" dependence of $\\langle N_{\\rm coll} \\rangle$ for the $\\rho$\nselection shows the smallest deviations ($<8$ %) with respect to that obtained\nusing impact parameter $b$; on the other hand, the V0M and CL1 yield huge\ndeviations (up to a factor 2) with respect to the results using $b$. The\nparticle ratios and nuclear modification factors ($Q_{\\rm pPb}$) as a function\nof $p_{\\rm T}$ are also studied. The proton-to-pion ratio exhibits a flow-like\npeak at intermediate $p_{\\rm T}$ (2-8 GeV/$c$) with little or no \"centrality\"\ndependence for V0M, $\\rho$ and $b$ selections. The kaon-to-pion ratio as a\nfunction of $p_{\\rm T}$ is \"centrality\" independent for the same selections. On\nthe contrary, for the CL1 class the ratios exhibit the typical behaviour\nassociated with hard physics. Regarding $Q_{\\rm pPb}$, a peak at intermediate\n$p_{\\rm T}$ ($2-8$ GeV/$c$) for different particle species is observed when the\n\"centrality\" is obtained with $b$ or $\\rho$. The observed features diminish for\nthe selections based on V0M and CL1.","PeriodicalId":501206,"journal":{"name":"arXiv - PHYS - Nuclear Experiment","volume":"69 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-07-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Flattenicity as \\\"centrality\\\" estimator in p-Pb collisions simulated with PYTHIA 8.312 Angantyr\",\"authors\":\"Antonio Ortiz, Gyula Bencedi, Feng Fan\",\"doi\":\"arxiv-2407.07724\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In this paper, a \\\"centrality\\\" estimator based on flattenicity ($\\\\rho$) is\\nstudied in proton-led (p-Pb) collisions at $\\\\sqrt{s_{\\\\rm NN}}=5.02$ TeV using\\nPYTHIA 8 Angantyr. Although Angantyr is still under development, the existing\\nimplementation is enough to study the particle production in systems where\\nmedium effects are absent. Firstly, ALICE data on pseudorapidity distributions\\nas a function of the forward multiplicity (V0M), as well as transverse momentum\\ndistributions of identified particles in non-single diffractive p-Pb\\ncollisions, are compared with Angantyr. Secondly, the average number of binary\\nnucleon-nucleon ($N_{\\\\rm coll}$) collisions for different \\\"centrality\\\"\\nestimators are compared. The studies include the following \\\"centrality\\\"\\nestimators: V0M, $\\\\rho$ and midrapidity multiplicity (CL1). On one hand, the\\n\\\"centrality\\\" dependence of $\\\\langle N_{\\\\rm coll} \\\\rangle$ for the $\\\\rho$\\nselection shows the smallest deviations ($<8$ %) with respect to that obtained\\nusing impact parameter $b$; on the other hand, the V0M and CL1 yield huge\\ndeviations (up to a factor 2) with respect to the results using $b$. The\\nparticle ratios and nuclear modification factors ($Q_{\\\\rm pPb}$) as a function\\nof $p_{\\\\rm T}$ are also studied. The proton-to-pion ratio exhibits a flow-like\\npeak at intermediate $p_{\\\\rm T}$ (2-8 GeV/$c$) with little or no \\\"centrality\\\"\\ndependence for V0M, $\\\\rho$ and $b$ selections. The kaon-to-pion ratio as a\\nfunction of $p_{\\\\rm T}$ is \\\"centrality\\\" independent for the same selections. On\\nthe contrary, for the CL1 class the ratios exhibit the typical behaviour\\nassociated with hard physics. Regarding $Q_{\\\\rm pPb}$, a peak at intermediate\\n$p_{\\\\rm T}$ ($2-8$ GeV/$c$) for different particle species is observed when the\\n\\\"centrality\\\" is obtained with $b$ or $\\\\rho$. The observed features diminish for\\nthe selections based on V0M and CL1.\",\"PeriodicalId\":501206,\"journal\":{\"name\":\"arXiv - PHYS - Nuclear Experiment\",\"volume\":\"69 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-07-10\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Nuclear Experiment\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2407.07724\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Nuclear Experiment","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2407.07724","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Flattenicity as "centrality" estimator in p-Pb collisions simulated with PYTHIA 8.312 Angantyr
In this paper, a "centrality" estimator based on flattenicity ($\rho$) is
studied in proton-led (p-Pb) collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV using
PYTHIA 8 Angantyr. Although Angantyr is still under development, the existing
implementation is enough to study the particle production in systems where
medium effects are absent. Firstly, ALICE data on pseudorapidity distributions
as a function of the forward multiplicity (V0M), as well as transverse momentum
distributions of identified particles in non-single diffractive p-Pb
collisions, are compared with Angantyr. Secondly, the average number of binary
nucleon-nucleon ($N_{\rm coll}$) collisions for different "centrality"
estimators are compared. The studies include the following "centrality"
estimators: V0M, $\rho$ and midrapidity multiplicity (CL1). On one hand, the
"centrality" dependence of $\langle N_{\rm coll} \rangle$ for the $\rho$
selection shows the smallest deviations ($<8$ %) with respect to that obtained
using impact parameter $b$; on the other hand, the V0M and CL1 yield huge
deviations (up to a factor 2) with respect to the results using $b$. The
particle ratios and nuclear modification factors ($Q_{\rm pPb}$) as a function
of $p_{\rm T}$ are also studied. The proton-to-pion ratio exhibits a flow-like
peak at intermediate $p_{\rm T}$ (2-8 GeV/$c$) with little or no "centrality"
dependence for V0M, $\rho$ and $b$ selections. The kaon-to-pion ratio as a
function of $p_{\rm T}$ is "centrality" independent for the same selections. On
the contrary, for the CL1 class the ratios exhibit the typical behaviour
associated with hard physics. Regarding $Q_{\rm pPb}$, a peak at intermediate
$p_{\rm T}$ ($2-8$ GeV/$c$) for different particle species is observed when the
"centrality" is obtained with $b$ or $\rho$. The observed features diminish for
the selections based on V0M and CL1.