{"title":"大型强子对撞机能量下的事件-事件粒子比波动","authors":"Shaista Khan, B. Ali, A. Chandra, S. Ahmad","doi":"10.1155/2021/6663846","DOIUrl":null,"url":null,"abstract":"<jats:p>A Monte Carlo study of identified particle ratio fluctuations at LHC energies is carried out in the framework of HIJING model using the fluctuation variable <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M1\">\n <msub>\n <mrow>\n <mi>ν</mi>\n </mrow>\n <mrow>\n <mtext>dyn</mtext>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula>. The simulated events for Pb-Pb collisions at <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M2\">\n <msub>\n <mrow>\n <msqrt>\n <mrow>\n <mi>s</mi>\n </mrow>\n </msqrt>\n </mrow>\n <mrow>\n <mi>N</mi>\n <mi>N</mi>\n </mrow>\n </msub>\n <mo>=</mo>\n <mn>2.76</mn>\n </math>\n </jats:inline-formula> and 5.02 TeV and Xe-Xe collisions at <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M3\">\n <msub>\n <mrow>\n <msqrt>\n <mrow>\n <mi>s</mi>\n </mrow>\n </msqrt>\n </mrow>\n <mrow>\n <mi>N</mi>\n <mi>N</mi>\n </mrow>\n </msub>\n <mo>=</mo>\n <mn>5.44</mn>\n <mtext> </mtext>\n <mtext>TeV</mtext>\n </math>\n </jats:inline-formula> are analyzed. From this study, it is observed that the values of <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M4\">\n <mfenced open=\"[\" close=\"]\">\n <mrow>\n <mi>π</mi>\n <mo>,</mo>\n <mi>K</mi>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula>, <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M5\">\n <mfenced open=\"[\" close=\"]\">\n <mrow>\n <mi>p</mi>\n <mo>,</mo>\n <mi>K</mi>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula>, and <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M6\">\n <mfenced open=\"[\" close=\"]\">\n <mrow>\n <mi>π</mi>\n <mo>,</mo>\n <mi>p</mi>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> follow the similar trends of energy dependence as observed in the most central collision data by NA49, STAR, and ALICE experiments. It is also observed that <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M7\">\n <msub>\n <mrow>\n <mi>ν</mi>\n </mrow>\n <mrow>\n <mtext>dyn</mtext>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula> for all the three combinations of particles for semicentral and central collisions, the model predicted values of <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M8\">\n <msub>\n <mrow>\n <mi>ν</mi>\n </mrow>\n <mrow>\n <mtext>dyn</mtext>\n </mrow>\n </msub>\n <mfenced open=\"[\" close=\"]\">\n <mrow>\n <mi>A</mi>\n <mo>,</mo>\n <mi>B</mi>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> for Pb-Pb collisions at <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M9\">\n <msub>\n <mrow>\n <msqrt>\n <mrow>\n <mi>s</mi>\n </mrow>\n </msqrt>\n </mrow>\n <mrow>\n <mi>N</mi>\n <mi>N</mi>\n </mrow>\n </msub>\n <mo>=</mo>\n <mn>2.76</mn>\n <mtext> </mtext>\n <mtext>TeV</mtext>\n </math>\n </jats:inline-formula> agree fairly well with those observed in the ALICE experiment. For peripheral collisions, however, the model predicted values of <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M10\">\n <msub>\n <mrow>\n <mi>ν</mi>\n </mrow>\n <mrow>\n <mtext>dyn</mtext>\n </mrow>\n </msub>\n <mfenced open=\"[\" close=\"]\">\n <mrow>\n <mi>π</mi>\n <mo>,</mo>\n <mi>K</mi>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> are somewhat smaller, whereas for <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M11\">\n <mfenced open=\"[\" close=\"]\">\n <mrow>\n <mi>p</mi>\n <mo>,</mo>\n <mi>K</mi>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> and <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M12\">\n <mfenced open=\"[\" close=\"]\">\n <mrow>\n <mi>π</mi>\n <mo>,</mo>\n <mi>p</mi>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> it predicts larger values as compared to the corresponding experimental values. The possible reasons for the observed differences are discussed. The <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M13\">\n <msub>\n <mrow>\n <mi>ν</mi>\n </mrow>\n <mrow>\n <mtext>dyn</mtext>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula> values scaled with charged particle density when plotted against <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M14\">\n <mfenced open=\"〈\" close=\"〉\">\n <mrow>\n <msub>\n <mrow>\n <mi>N</mi>\n </mrow>\n <mrow>\n <mtext>part</mtext>\n </mrow>\n </msub>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> exhibit a flat behaviour, as expected from the independent particle emission sources. For <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M15\">\n <mfenced open=\"[\" close=\"]\">\n <mrow>\n <mi>p</mi>\n <mo>,</mo>\n <mi>K</mi>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> and <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M16\">\n <mfenced open=\"[\" close=\"]\">\n <mrow>\n <mi>π</mi>\n <mo>,</mo>\n ","PeriodicalId":7498,"journal":{"name":"Advances in High Energy Physics","volume":" ","pages":""},"PeriodicalIF":1.5000,"publicationDate":"2021-08-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Event-by-Event Particle Ratio Fluctuations at LHC Energies\",\"authors\":\"Shaista Khan, B. Ali, A. Chandra, S. Ahmad\",\"doi\":\"10.1155/2021/6663846\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<jats:p>A Monte Carlo study of identified particle ratio fluctuations at LHC energies is carried out in the framework of HIJING model using the fluctuation variable <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M1\\\">\\n <msub>\\n <mrow>\\n <mi>ν</mi>\\n </mrow>\\n <mrow>\\n <mtext>dyn</mtext>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula>. The simulated events for Pb-Pb collisions at <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M2\\\">\\n <msub>\\n <mrow>\\n <msqrt>\\n <mrow>\\n <mi>s</mi>\\n </mrow>\\n </msqrt>\\n </mrow>\\n <mrow>\\n <mi>N</mi>\\n <mi>N</mi>\\n </mrow>\\n </msub>\\n <mo>=</mo>\\n <mn>2.76</mn>\\n </math>\\n </jats:inline-formula> and 5.02 TeV and Xe-Xe collisions at <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M3\\\">\\n <msub>\\n <mrow>\\n <msqrt>\\n <mrow>\\n <mi>s</mi>\\n </mrow>\\n </msqrt>\\n </mrow>\\n <mrow>\\n <mi>N</mi>\\n <mi>N</mi>\\n </mrow>\\n </msub>\\n <mo>=</mo>\\n <mn>5.44</mn>\\n <mtext> </mtext>\\n <mtext>TeV</mtext>\\n </math>\\n </jats:inline-formula> are analyzed. From this study, it is observed that the values of <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M4\\\">\\n <mfenced open=\\\"[\\\" close=\\\"]\\\">\\n <mrow>\\n <mi>π</mi>\\n <mo>,</mo>\\n <mi>K</mi>\\n </mrow>\\n </mfenced>\\n </math>\\n </jats:inline-formula>, <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M5\\\">\\n <mfenced open=\\\"[\\\" close=\\\"]\\\">\\n <mrow>\\n <mi>p</mi>\\n <mo>,</mo>\\n <mi>K</mi>\\n </mrow>\\n </mfenced>\\n </math>\\n </jats:inline-formula>, and <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M6\\\">\\n <mfenced open=\\\"[\\\" close=\\\"]\\\">\\n <mrow>\\n <mi>π</mi>\\n <mo>,</mo>\\n <mi>p</mi>\\n </mrow>\\n </mfenced>\\n </math>\\n </jats:inline-formula> follow the similar trends of energy dependence as observed in the most central collision data by NA49, STAR, and ALICE experiments. It is also observed that <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M7\\\">\\n <msub>\\n <mrow>\\n <mi>ν</mi>\\n </mrow>\\n <mrow>\\n <mtext>dyn</mtext>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula> for all the three combinations of particles for semicentral and central collisions, the model predicted values of <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M8\\\">\\n <msub>\\n <mrow>\\n <mi>ν</mi>\\n </mrow>\\n <mrow>\\n <mtext>dyn</mtext>\\n </mrow>\\n </msub>\\n <mfenced open=\\\"[\\\" close=\\\"]\\\">\\n <mrow>\\n <mi>A</mi>\\n <mo>,</mo>\\n <mi>B</mi>\\n </mrow>\\n </mfenced>\\n </math>\\n </jats:inline-formula> for Pb-Pb collisions at <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M9\\\">\\n <msub>\\n <mrow>\\n <msqrt>\\n <mrow>\\n <mi>s</mi>\\n </mrow>\\n </msqrt>\\n </mrow>\\n <mrow>\\n <mi>N</mi>\\n <mi>N</mi>\\n </mrow>\\n </msub>\\n <mo>=</mo>\\n <mn>2.76</mn>\\n <mtext> </mtext>\\n <mtext>TeV</mtext>\\n </math>\\n </jats:inline-formula> agree fairly well with those observed in the ALICE experiment. For peripheral collisions, however, the model predicted values of <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M10\\\">\\n <msub>\\n <mrow>\\n <mi>ν</mi>\\n </mrow>\\n <mrow>\\n <mtext>dyn</mtext>\\n </mrow>\\n </msub>\\n <mfenced open=\\\"[\\\" close=\\\"]\\\">\\n <mrow>\\n <mi>π</mi>\\n <mo>,</mo>\\n <mi>K</mi>\\n </mrow>\\n </mfenced>\\n </math>\\n </jats:inline-formula> are somewhat smaller, whereas for <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M11\\\">\\n <mfenced open=\\\"[\\\" close=\\\"]\\\">\\n <mrow>\\n <mi>p</mi>\\n <mo>,</mo>\\n <mi>K</mi>\\n </mrow>\\n </mfenced>\\n </math>\\n </jats:inline-formula> and <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M12\\\">\\n <mfenced open=\\\"[\\\" close=\\\"]\\\">\\n <mrow>\\n <mi>π</mi>\\n <mo>,</mo>\\n <mi>p</mi>\\n </mrow>\\n </mfenced>\\n </math>\\n </jats:inline-formula> it predicts larger values as compared to the corresponding experimental values. The possible reasons for the observed differences are discussed. The <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M13\\\">\\n <msub>\\n <mrow>\\n <mi>ν</mi>\\n </mrow>\\n <mrow>\\n <mtext>dyn</mtext>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula> values scaled with charged particle density when plotted against <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M14\\\">\\n <mfenced open=\\\"〈\\\" close=\\\"〉\\\">\\n <mrow>\\n <msub>\\n <mrow>\\n <mi>N</mi>\\n </mrow>\\n <mrow>\\n <mtext>part</mtext>\\n </mrow>\\n </msub>\\n </mrow>\\n </mfenced>\\n </math>\\n </jats:inline-formula> exhibit a flat behaviour, as expected from the independent particle emission sources. For <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M15\\\">\\n <mfenced open=\\\"[\\\" close=\\\"]\\\">\\n <mrow>\\n <mi>p</mi>\\n <mo>,</mo>\\n <mi>K</mi>\\n </mrow>\\n </mfenced>\\n </math>\\n </jats:inline-formula> and <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M16\\\">\\n <mfenced open=\\\"[\\\" close=\\\"]\\\">\\n <mrow>\\n <mi>π</mi>\\n <mo>,</mo>\\n \",\"PeriodicalId\":7498,\"journal\":{\"name\":\"Advances in High Energy Physics\",\"volume\":\" \",\"pages\":\"\"},\"PeriodicalIF\":1.5000,\"publicationDate\":\"2021-08-11\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Advances in High Energy Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1155/2021/6663846\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, PARTICLES & FIELDS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advances in High Energy Physics","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1155/2021/6663846","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, PARTICLES & FIELDS","Score":null,"Total":0}
引用次数: 1
摘要
在HIJING模型的框架下,使用波动变量Γdyn对LHC能量下已识别的粒子比波动进行了蒙特卡罗研究。s N N下Pb-Pb碰撞的模拟事件=2.76和5.02 sN下的TeV和XeXe碰撞=5.44 对TeV进行了分析。从这项研究中可以观察到π、K,p、K和π,p遵循与NA49、STAR和ALICE实验在最中心碰撞数据中观察到的能量依赖性相似的趋势。还观察到,对于半中心和中心碰撞的所有三种粒子组合,Δ的模型预测值,Pb与Pb碰撞的BN N=2.76 TeV与ALICE实验中观察到的结果相当吻合。
Event-by-Event Particle Ratio Fluctuations at LHC Energies
A Monte Carlo study of identified particle ratio fluctuations at LHC energies is carried out in the framework of HIJING model using the fluctuation variable . The simulated events for Pb-Pb collisions at and 5.02 TeV and Xe-Xe collisions at are analyzed. From this study, it is observed that the values of , , and follow the similar trends of energy dependence as observed in the most central collision data by NA49, STAR, and ALICE experiments. It is also observed that for all the three combinations of particles for semicentral and central collisions, the model predicted values of for Pb-Pb collisions at agree fairly well with those observed in the ALICE experiment. For peripheral collisions, however, the model predicted values of are somewhat smaller, whereas for and it predicts larger values as compared to the corresponding experimental values. The possible reasons for the observed differences are discussed. The values scaled with charged particle density when plotted against exhibit a flat behaviour, as expected from the independent particle emission sources. For and
期刊介绍:
Advances in High Energy Physics publishes the results of theoretical and experimental research on the nature of, and interaction between, energy and matter. Considering both original research and focussed review articles, the journal welcomes submissions from small research groups and large consortia alike.