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dS2 supergravity
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Abstract
We construct two-dimensional supergravity theories endowed with a positive cosmological constant, that admit de Sitter vacua. We consider the cases of $$ \mathcal{N} $$
N
= 1 as well as $$ \mathcal{N} $$
N
= 2 supersymmetry, and couple the supergravity to a superconformal field theory with the same amount of supersymmetry. Upon fixing a supersymmetric extension of the Weyl gauge, the theories are captured, at the quantum level, by supersymmetric extensions of timelike Liouville theory with $$ \mathcal{N} $$
N
= 1 and $$ \mathcal{N} $$
N
= 2 supersymmetry respectively. The theories exhibit good ultraviolet properties and are amenable to a variety of techniques such as systematic loop expansions and, in the $$ \mathcal{N} $$
N
= 2 case, supersymmetric localization. Our constructions offer a novel path toward a precise treatment of the Euclidean gravitational path integral for de Sitter, and in turn, the Gibbons-Hawking entropy of the de Sitter horizon. We argue that the supersymmetric localization method applied to the $$ \mathcal{N} $$
N
= 2 theory must receive contributions from boundary terms in configuration space. We also discuss how these theories overcome several obstructions that appear upon combining de Sitter space with supersymmetry.
Springer Science and Business Media LLC
Title: dS2 supergravity
Description:
Abstract
We construct two-dimensional supergravity theories endowed with a positive cosmological constant, that admit de Sitter vacua.
We consider the cases of $$ \mathcal{N} $$
N
= 1 as well as $$ \mathcal{N} $$
N
= 2 supersymmetry, and couple the supergravity to a superconformal field theory with the same amount of supersymmetry.
Upon fixing a supersymmetric extension of the Weyl gauge, the theories are captured, at the quantum level, by supersymmetric extensions of timelike Liouville theory with $$ \mathcal{N} $$
N
= 1 and $$ \mathcal{N} $$
N
= 2 supersymmetry respectively.
The theories exhibit good ultraviolet properties and are amenable to a variety of techniques such as systematic loop expansions and, in the $$ \mathcal{N} $$
N
= 2 case, supersymmetric localization.
Our constructions offer a novel path toward a precise treatment of the Euclidean gravitational path integral for de Sitter, and in turn, the Gibbons-Hawking entropy of the de Sitter horizon.
We argue that the supersymmetric localization method applied to the $$ \mathcal{N} $$
N
= 2 theory must receive contributions from boundary terms in configuration space.
We also discuss how these theories overcome several obstructions that appear upon combining de Sitter space with supersymmetry.
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