Euclidean wormholes in holographic RG flows

IF 5.4 1区 物理与天体物理 Q1 Physics and Astronomy Journal of High Energy Physics Pub Date : 2024-11-15 DOI:10.1007/JHEP11(2024)096
Jeevan Chandra
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Abstract

We describe a one-parameter family of Euclidean wormhole solutions with the topology of a compact hyperbolic space times an interval in Einstein gravity minimally coupled to a massless scalar field in AdSd+1 commonly referred to as Einstein-dilaton gravity. These solutions are locally described by the same metric and dilaton profile as the single-boundary Janus domain wall solutions in the same theory which are usually studied in the context of holographic RG flows. The wormholes compute the averaged product of partition functions of CFTs on either boundary deformed by different marginal couplings to the scalar operator dual to the dilaton. We observe that the renormalised volumes of these wormholes increase monotonically with the difference in the marginal couplings on the boundary thereby showing that the pair of CFTs on the boundaries get increasingly decorrelated as the difference in the marginal couplings increases. We use the partition functions of the three-dimensional wormhole solutions to determine the variance of the OPE data of local operators between the marginally deformed 2d CFTs and quantify how the variance decays with the difference in marginal couplings. In addition, a family of wormholes sourced by a thin shell of dust determine how the variance of the matrix elements of the dual line defect decays with the difference in marginal couplings. Applying the GKPW dictionary to wormholes, we compute averages of integrated dilaton correlators treating the wormhole amplitude as a functional of the dilaton sources. We observe that the crossed two-point correlators with a dilaton insertion on either boundary decay monotonically with the difference in marginal couplings consistent with the observation that the CFTs increasingly decorrelate as the difference in marginal couplings grows.

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全息 RG 流中的欧式虫洞
我们描述了一个欧几里得虫洞解的单参数族,其拓扑结构是紧凑双曲空间乘以爱因斯坦引力最小耦合 AdSd+1 无质量标量场的区间,通常称为爱因斯坦稀拉顿引力。这些解的局部度量和稀拉顿轮廓与同一理论中的单边界杰纳斯域壁解所描述的度量和稀拉顿轮廓相同,后者通常在全息 RG 流的背景下进行研究。虫洞计算的是任一边界上由与稀拉顿对偶的标量算子的不同边际耦合变形的 CFT 的分割函数的平均乘积。我们观察到,这些虫洞的重规范化体积随着边界上边际耦合的差异而单调增加,从而表明随着边际耦合差异的增加,边界上的一对 CFT 越来越不相关。我们利用三维虫洞解的分区函数来确定边际变形二维CFT之间局部算子的OPE数据方差,并量化了方差如何随边际耦合的差异而衰减。此外,由尘埃薄壳产生的虫洞家族确定了双线缺陷矩阵元素的方差如何随边际耦合的不同而衰减。将 GKPW 字典应用于虫洞,我们计算了将虫洞振幅视为稀释源函数的积分稀释相关器的平均值。我们观察到,在任一边界上插入稀释子的交叉两点相关器会随着边际耦合差的增大而单调衰减,这与随着边际耦合差的增大而CFT越来越去相关的观察结果是一致的。
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来源期刊
Journal of High Energy Physics
Journal of High Energy Physics 物理-物理:粒子与场物理
CiteScore
10.30
自引率
46.30%
发文量
2107
审稿时长
1.5 months
期刊介绍: The aim of the Journal of High Energy Physics (JHEP) is to ensure fast and efficient online publication tools to the scientific community, while keeping that community in charge of every aspect of the peer-review and publication process in order to ensure the highest quality standards in the journal. Consequently, the Advisory and Editorial Boards, composed of distinguished, active scientists in the field, jointly establish with the Scientific Director the journal''s scientific policy and ensure the scientific quality of accepted articles. JHEP presently encompasses the following areas of theoretical and experimental physics: Collider Physics Underground and Large Array Physics Quantum Field Theory Gauge Field Theories Symmetries String and Brane Theory General Relativity and Gravitation Supersymmetry Mathematical Methods of Physics Mostly Solvable Models Astroparticles Statistical Field Theories Mostly Weak Interactions Mostly Strong Interactions Quantum Field Theory (phenomenology) Strings and Branes Phenomenological Aspects of Supersymmetry Mostly Strong Interactions (phenomenology).
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Euclidean wormholes in holographic RG flows Addendum to: Combined analysis of neutrino decoherence at reactor experiments Toward double copy on arbitrary backgrounds Revisiting the minimal Nelson-Barr model Interpretations of the ATLAS measurements of Higgs boson production and decay rates and differential cross-sections in pp collisions at \( \sqrt{s} \) = 13 TeV
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