A path integral realization of joint <inline-formula id='IEq1'> <alternatives> <mml:math display='inline'> <mml:mi>J</mml:mi> <mml:mover accent='true'> <mml:mi>T</mml:mi> <mml:mo stretchy='true'>ˉ</mml:mo> </mml:mover> </mml:math> <tex-math id='IEq1_TeX'>documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ Joverline{T} $$end{document}</tex-math> <inline-graphic xlink:href='13130_2020_13369_Article_IEq1.gif'/> </alternatives> </inline-formula>, <inline-formula id='IEq2'> <alternatives> <mml:math display='inline'> <mml:mi>T</mml:mi> <mml:mover accent='true'> <mml:mi>J</mml:mi> <mml:mo stretchy='true'>ˉ</mml:mo> </mml:mover> </mml:math> <tex-math id='IEq2_TeX'>documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ Toverline{J} $$end{document}</tex-math> <inline-graphic xlink:href='13130_2020_13369_Article_IEq2.gif'/> </alternatives> </inline-formula> and <inline-formula id='IEq3'> <alternatives> <mml:math display='inline'> <mml:mi>T</mml:mi> <mml:mover accent='true'> <mml:mi>T</mml:mi> <mml:mo stretchy='true'>ˉ</mml:mo> </mml:mover> </mml:math> <tex-math id='IEq3_TeX'>documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ Toverline{T} $$end{document}</tex-math> <inline-graphic xlink:href='13130_2020_13369_Article_IEq3.gif'/> </alternatives> </inline-formula> flows

Jeremías Aguilera-Damia; Victor I. Giraldo-Rivera; Edward A. Mazenc; Ignacio Salazar Landea; Ronak M Soni

首页> 外文期刊>The journal of high energy physics >A path integral realization of joint 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}$$ Joverline{T} $$end{document}

, T J ˉ

and T T ˉ

flows

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A path integral realization of joint 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}$$ Joverline{T} $$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}$$ Toverline{J} $$end{document} and 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}$$ Toverline{T} $$end{document} flows

机译：关节 <替代方案> j t ˉ documentClass [12pt] {minimal} usepackage {ammath} usepackage {keysym} usepackage {amsfonts} usepackage {amssymb} usepackage {amsbsy} usepackage {mathrsfs} usepackage {supmeek} setLength { oddsidemargin } { - 69pt} begin {document} $$ j overline {t} $$ end {document} ，<内联公式id =“IEQ2”> <替代方案> t j ˉ DocumentClass [12pt] {minimal} usepackage {ammath} usepackage {isysym} usepackage {amsfonts} usepackage {amssymb} usepackage {amsbsy} usepackage {mathrsf s} usepackage {supmeez} setLength { oddsidemargin} { - 69pt} begin {document} $$ t overline {j} $$ end {document} 和 t T ˉ < / mml：math> documentClass [12pt] {minimal} usepackage {ammath} usepackage {isysym} usepackage {amsfonts} usepackage {amssymb} usepackage {amsbsy} usepackage {mathrsfs} usepackage {supmeek} setLength { oddsidemargin} { - 69pt} begin {document} $$ t overline {t} $$ end {document} 流

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A bstract We recast the joint 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}$$ Joverline{T} $$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}$$ Toverline{J} $$end{document} and 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}$$ Toverline{T} $$end{document} deformations as coupling the original theory to a mixture of topological gravity and gauge theory. This geometrizes the general flow triggered by irrelevant deformations built out of conserved currents and the stress-energy tensor, by means of a path integral kernel. The partition function of the deformed theory satisfies a diffusion-like flow equation similar to that found in the pure 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}$$ Toverline{T} $$end{document} case. Our proposal passes two stringent tests. Firstly, we recover the classical deformed actions from the kernel, reproducing the known expressions for the free boson and fermion. Secondly, we explicitly compute the torus path integral along the flow and show it localizes to a finite-dimensional, one-loop exact integral over base space torus moduli. The dressed energy levels so obtained match exactly onto those previously reported in the literature.

机译：Bstract我们重新开始关节JTˉ DocumentClass [12pt] {minimal} usepackage {ammath} usepackage {isysym} usepackage {amsfonts} usepackage {amsbsy} usepackage {mathrsfs} usepackage {supmeek } setLength { oddsidemargin} { - 69pt} begin {document} $$ j overline {t} $$ end {document}，tjˉ documentclass [12pt] {minimal} usepackage {ammath} usepackage { visiSym} usemackage {amsfonts} usepackage {amssymb} usepackage {amsbsy} usepackage {mathrsfs} usepackage {supmeek} setLength { oddsideDemargin} { - 69pt} begin {document} $$ t overline {j} $$。 {升级} setLength { oddsidemargin} { - 69pt} begin {document} $$ t overline {document} $$ end {document}变形是将原始理论耦合到拓扑重力和仪表理论的混合。这种通过路径积分内核构成由保守电流和应力 - 能量张量构成的无关变形引发的一般流动。变形理论的分区函数满足类似于纯TTˉ documentClass [12pt] {minimal} usepackage {ammath} usepackage {isysym} usepackage {amsfonts} usepackage {amsyymb的流量方程} usepackage {amsbsy} usepackage {mathrsfs} usepackage {supmeek} setLength { oddsidemargin} { - 69pt} begin {document} $$ t overline {t} $$ end {document}案例。我们的提议通过了两个严格的测试。首先，我们从内核中恢复了经典的变形动作，再现了免费玻色子和费米的已知表达。其次，我们明确地计算沿着流程的整体圆环路径，并将其定位为碱基空间圆环模数的有限维度，单环精确整体。衣服的能量水平如此获得的匹配与先前在文献中报道的那些相匹配。

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《The journal of high energy physics》 |2020年第7期|共43页
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Jeremías Aguilera-Damia; Victor I. Giraldo-Rivera; Edward A. Mazenc; Ignacio Salazar Landea; Ronak M Soni;
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2D GravityField Theories in Lower DimensionsNonperturbative Effects;

机译：2D重力场理论较低尺寸无扰动效应;
入库时间 2022-08-19 02:13:47

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1. Thermodynamics of 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 conformal field theories [J] . Soumangsu Chakraborty, Akikazu Hashimoto The journal of high energy physics . 2020,第7期

机译：<内联公式ID =“IEQ1”> <替代品> T t ˉ DocumentClass [12pt] {minimal} usepackage {ammath} usepackage {isysym} usepackage {amsfonts} usepackage {amssys} usepackage {mathrsfs} usepackage {mathrsfs} usepackage {supbeek } setLength { oddsidemargin} { - 69pt} begin {document} $$ mathrm {t} overline { mathrm {t}} $$ end {document} <内联图xlink ：href =“13130_2020_13473_ARTICLICLE_IEQ1.gif”/> ， Ĵ T ˉ< / mml：mo> DocumentClass [12pt] {minimal} usepackage {ammath} usepackage {keysym} usepackage {amsfonts} usepackage {amssymb} usepackage {amsbsy} usepackage {mathrsfs} usepackage {supmeek} setLength { oddsideDemargin} {-69pt} begin {document} $$$$ mathrm {j} overline { $$ end {document} ，<内联公式id =“IEQ3”> <替代方案> T J ˉ 的DocumentClass [12磅] {最小} usepackage {amsmath} usepackage {wasysym} usepackage {amsfonts} usepackage {amssymb} usepackage {amsbsy} usepackage {mathrsfs} usepackage {upgreek} setlength { oddsidemargin} {-69pt} begin {document} $$ mathrm {t} overline { mathrm {t}} $$ end {document} 变形的保形磁场领域IES.
2. 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 [J] . Soumangsu Chakraborty, Akikazu Hashimoto The journal of high energy physics . 2021,第2期

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
3. Top-induced contributions to H → b b ˉ documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ boverline{b} $$end{document} and H → c c ˉ documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ coverline{c} $$end{document} at O α s 3 documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ mathcal{O}left({lpha}_s^3ight) $$end{document} [J] . Roberto Mondini, Ulrich Schubert, Ciaran Williams The journal of high energy physics . 2020,第12期

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4. Evidence of bar Minigene Expression and \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} \begin{equation*}tRNA_{2}^{Ile}\end{equation*}\end{document}Sequestration as \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} \begin{equation*}Peptidyl-tRNA_{2}^{{\mathrm{Ile}}}\end{equation*}\end{document}during Lambda Bacteriophage Development [O] . Oviedo de Anda, Norma Angélica, Kameyama, Luis, Galindo, José Manuel, 2004

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