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弦理论中的对称薄膜晶体管。

Symmetry TFTs from String Theory.

作者信息

Apruzzi Fabio, Bonetti Federico, García Etxebarria Iñaki, Hosseini Saghar S, Schäfer-Nameki Sakura

机构信息

Albert Einstein Center for Fundamental Physics, Institute for Theoretical Physics, University of Bern, Sidlerstrasse 5, Bern, 3012 Switzerland.

Mathematical Institute, University of Oxford, Andrew-Wiles Building, Woodstock Road, Oxford, OX2 6GG UK.

出版信息

Commun Math Phys. 2023;402(1):895-949. doi: 10.1007/s00220-023-04737-2. Epub 2023 May 26.

DOI:10.1007/s00220-023-04737-2
PMID:37475876
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10353977/
Abstract

We determine the dimensional topological field theory, which encodes the higher-form symmetries and their 't Hooft anomalies for -dimensional QFTs obtained by compactifying M-theory on a non-compact space . The resulting theory, which we call the Symmetry TFT, or SymTFT for short, is derived by reducing the topological sector of 11d supergravity on the boundary of the space . Central to this endeavour is a reformulation of supergravity in terms of differential cohomology, which allows the inclusion of torsion in cohomology of the space , which in turn gives rise to the background fields for discrete (in particular higher-form) symmetries. We apply this framework to 7d super-Yang Mills, where , as well as the Sasaki-Einstein links of Calabi-Yau three-fold cones that give rise to 5d superconformal field theories. This M-theory analysis is complemented with a IIB 5-brane web approach, where we derive the SymTFTs from the asymptotics of the 5-brane webs. Our methods apply to both Lagrangian and non-Lagrangian theories, and allow for many generalisations.

摘要

我们确定了维度拓扑场论,它编码了通过在非紧致空间上紧致化M理论得到的d维量子场论的高阶形式对称性及其‘t Hooft反常。由此产生的理论,我们简称为对称拓扑场论(SymTFT),是通过在空间的边界上约化11维超引力的拓扑部分而导出的。这项工作的核心是根据微分上同调对超引力进行重新表述,这允许在空间的上同调中包含挠率,进而产生离散(特别是高阶形式)对称性的背景场。我们将这个框架应用于7维超杨-米尔斯理论,以及产生5维超共形场论的卡拉比-丘三维锥的萨斯卡-爱因斯坦联系。这种M理论分析辅以IIB 5膜网方法,我们从5膜网的渐近性中导出对称拓扑场论。我们的方法适用于拉格朗日理论和非拉格朗日理论,并允许进行许多推广。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d966/10353977/ff80500e4b30/220_2023_4737_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d966/10353977/b6978a135b00/220_2023_4737_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d966/10353977/a643c01606d6/220_2023_4737_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d966/10353977/8d5571408778/220_2023_4737_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d966/10353977/ff80500e4b30/220_2023_4737_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d966/10353977/b6978a135b00/220_2023_4737_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d966/10353977/a643c01606d6/220_2023_4737_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d966/10353977/8d5571408778/220_2023_4737_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d966/10353977/ff80500e4b30/220_2023_4737_Fig4_HTML.jpg

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