{"title":"晶格QCD在有限T和μ下的结果","authors":"Z. Fodor, S. Katz","doi":"10.1556/APH.18.2003.1.5","DOIUrl":null,"url":null,"abstract":"We propose a method to study lattice QCD at finite temperature (T) and chemical potential (μ). We test the method and compare it with the Glasgow method using nf = 4 staggered QCD with imaginary μ. The critical endpoint (E) of QCD on the Re(μ) —T plane is located. We use nf = 2 + 1 dynamical staggered quarks with semi-realistic masses on Lt = 4 lattices. Our results are based on \\({\\mathcal{O}}\\)(103 – 104) configurations.","PeriodicalId":7004,"journal":{"name":"Acta Physica Hungarica","volume":"54 1","pages":"41-48"},"PeriodicalIF":0.0000,"publicationDate":"2002-04-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"4","resultStr":"{\"title\":\"Lattice QCD results at finite T and μ\",\"authors\":\"Z. Fodor, S. Katz\",\"doi\":\"10.1556/APH.18.2003.1.5\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We propose a method to study lattice QCD at finite temperature (T) and chemical potential (μ). We test the method and compare it with the Glasgow method using nf = 4 staggered QCD with imaginary μ. The critical endpoint (E) of QCD on the Re(μ) —T plane is located. We use nf = 2 + 1 dynamical staggered quarks with semi-realistic masses on Lt = 4 lattices. Our results are based on \\\\({\\\\mathcal{O}}\\\\)(103 – 104) configurations.\",\"PeriodicalId\":7004,\"journal\":{\"name\":\"Acta Physica Hungarica\",\"volume\":\"54 1\",\"pages\":\"41-48\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2002-04-29\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"4\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Acta Physica Hungarica\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1556/APH.18.2003.1.5\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Acta Physica Hungarica","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1556/APH.18.2003.1.5","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
We propose a method to study lattice QCD at finite temperature (T) and chemical potential (μ). We test the method and compare it with the Glasgow method using nf = 4 staggered QCD with imaginary μ. The critical endpoint (E) of QCD on the Re(μ) —T plane is located. We use nf = 2 + 1 dynamical staggered quarks with semi-realistic masses on Lt = 4 lattices. Our results are based on \({\mathcal{O}}\)(103 – 104) configurations.