首页> 外文期刊>The journal of high energy physics >Entanglement entropy for T T ˉ documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ mathrm{T}overline{mathrm{T}} $$end{document} , J T ˉ documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ mathrm{J}overline{mathrm{T}} $$end{document} , T J ˉ documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ mathrm{T}overline{mathrm{J}} $$end{document} deformed holographic CFT
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Entanglement entropy for T T ˉ documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ mathrm{T}overline{mathrm{T}} $$end{document} , J T ˉ documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ mathrm{J}overline{mathrm{T}} $$end{document} , T J ˉ documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ mathrm{T}overline{mathrm{J}} $$end{document} deformed holographic CFT

机译:为<直列式ID = “IEq1”> <替代>纠缠熵 T T ˉ < TEX-数学ID = “IEq1_TeX”> 的DocumentClass [12磅] {最小} usepackage {amsmath} usepackage {wasysym} usepackage {amsfonts} usepackage {amssymb} usepackage {amsbsy} usepackage {mathrsfs} usepackage { upgreek} setlength { oddsidemargin} { - 69pt} {开始文档} $$ mathrm【T} {划线 mathrm【T}} $$ {端文档} <直列图形的xlink:HREF = “MediaObjects / 13130__14822_IEq1.gif”/> ,<直列式ID = “IEq2”> <替代> Ĵ T ˉ 的DocumentClass [12磅] {最小} {usepackage amsmath} {usepackage wasysym} {usepackage amsfonts} {usepackage amssymb} {usepackage amsbsy} {usepackage mathrsfs} {usepackage upgreek} setlength { oddsidemargin} { - 69pt} {开始文档} $$ mathrm {Ĵ} 上划线{ mathrm【T}} $$ {端文档} <直列图形的xlink:HREF = “MediaObjects / 13130__14822_IEq2.gif”/> ,<直列式ID = “IEq3”> <替代> T < MML:MI mathvariant = “正常”>Ĵ ˉ 的DocumentClass [12磅] {最小} usepackage {amsmath} usepackage {wasysym} usepackage {amsfonts} usepackage {amssymb} usepackage {amsbsy} usepackage {mathrsfs} usepackage {upgreek} setlength { oddsidemargin} { - 69pt} {开始文档} $$ mathrm【T} {划线 mathrm {Ĵ}} $$ {端文档} <直列图形的xlink:HREF = “MediaObjects / 13130__14822_IEq3.gif”/> 变形全息CFT

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A bstract We derive the geodesic equation for determining the Ryu-Takayanagi surface in AdS _(3)deformed by single trace μT T ˉ documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ mu Toverline{T} $$end{document} + ε + J T ˉ documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ {arepsilon}_{+}Joverline{T} $$end{document} + ε ? T J ˉ documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ {arepsilon}_{-}Toverline{J} $$end{document} deformation for generic values of ( μ, ε _(+) , ε _( ? )) for which the background is free of singularities. For generic values of ε _( ± ), Lorentz invariance is broken, and the Ryu-Takayanagi surface embeds non-trivially in time as well as spatial coordinates. We solve the geodesic equation and characterize the UV and IR behavior of the entanglement entropy and the Casini-Huerta c -function. We comment on various features of these observables in the ( μ, ε _(+) , ε _( ? )) parameter space. We discuss the matching at leading order in small ( μ, ε _(+) , ε _( ? )) expansion of the entanglement entropy between the single trace deformed holographic system and a class of double trace deformed theories where a strictly field theoretic analysis is possible. We also comment on expectation value of a large rectangular Wilson loop-like observable.
机译:甲bstract我们推导出短程线方程中的广告确定柳-高柳表面_(3)由单一微量变形μTŤˉ的DocumentClass [12磅] {最小} usepackage {amsmath} usepackage {wasysym} usepackage {amsfonts} usepackage {amssymb} {usepackage amsbsy} {usepackage mathrsfs} {usepackage upgreek} setlength { oddsidemargin} { - 69pt} {开始文档} $$ 亩Ť划线横置$$ {端文档} +ε+ JTˉ的DocumentClass [12磅] {最小} usepackage {amsmath} usepackage {wasysym} usepackage {amsfonts} usepackage {amssymb} usepackage {amsbsy} usepackage {mathrsfs} usepackage {upgreek} setlength { oddsidemargin} { - 69pt} {开始文档} $$ { varepsilon} _ {+} J□划线横置$$ {端文档} +ε? TJˉ的DocumentClass [12磅] {最小} usepackage {amsmath} usepackage {wasysym} usepackage {amsfonts} usepackage {amssymb} usepackage {amsbsy} usepackage {mathrsfs} usepackage {upgreek} setlength { oddsidemargin } { - 69pt} {开始文档} $$ { varepsilon} _ { - }Ť {划线}Ĵ$$ {端文档}变形为的一般值(μ,ε_(+),ε_( ?))该背景是免费的奇点。为ε的通用值_(±),洛伦兹不变性打破,柳-高柳表面嵌入非平凡在时间以及空间坐标。我们解决了测地线方程和表征纠缠熵和卡西尼 - 韦尔塔Ç - 函数的紫外线和红外线的行为。我们对在这些观测的各种功能评论(μ,ε_(+),ε_(?))参数空间。我们在小在领头阶讨论的匹配(μ,ε_(+),ε_(?))的单个迹线之间的纠缠熵的膨胀而变形的全息系统和一类双踪变形理论的其中一个严格场理论分析是可能的。我们还对大的矩形Wilson圈状的可观测的期望值评论。

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