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DSSYK at infinite temperature: the flat-space limit and the ’t Hooft model
DSSYK at infinite temperature: the flat-space limit and the ’t Hooft model
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DSSYK at infinite temperature: the flat-space limit and the ’t Hooft model
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DSSYK at infinite temperature: the flat-space limit and the ’t Hooft model
DSSYK at infinite temperature: the flat-space limit and the ’t Hooft model

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DSSYK at infinite temperature: the flat-space limit and the ’t Hooft model
DSSYK at infinite temperature: the flat-space limit and the ’t Hooft model
Journal Article

DSSYK at infinite temperature: the flat-space limit and the ’t Hooft model

2025
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Overview
A bstract In the limit of infinite radius de Sitter space becomes locally flat and the static patch tends to Rindler space. A holographic description of the static patch must result in a holographic description of some flat space theory, expressed in Rindler coordinates. Given such a holographic theory how does one decode the hologram and determine the bulk flat space theory, its particle spectrum, forces, and bulk quantum fields? In this paper we will answer this question for a particular case: DSSYK at infinite temperature and show that the bulk theory is a strongly coupled version of the ’t Hooft model, i.e., (1+1)-dimensional QCD, with a single quark flavor. It may also be thought of as an open string theory with mesons lying on a single Regge trajectory.