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Character integral representation of zeta function in AdS d+1 . Part II. Application to partially-massless higher-spin gravities

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TLDR
In this paper, the one-loop free energies of the type-Al and type-Bl higher-spin gravities in (d + 1)-dimensional anti-de Sitter (AdSd+1) spacetime were computed.
Abstract
We compute the one-loop free energies of the type-Al and type-Bl higher-spin gravities in (d + 1)-dimensional anti-de Sitter (AdSd+1) spacetime. For large d and l, these theories have a complicated field content, and hence it is difficult to compute their zeta functions using the usual methods. Applying the character integral representation of zeta function developed in the companion paper [ arXiv:1805.05646 ] to these theories, we show how the computation of their zeta function can be shortened considerably. We find that the results previously obtained for the massless theories (l = 1) generalize to their partially-massless counterparts (arbitrary l) in arbitrary dimensions.

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Quantum de Sitter horizon entropy from quasicanonical bulk, edge, sphere and topological string partition functions

TL;DR: In this paper, the exact one-loop corrected de Sitter entropy (the logarithm of the sphere partition function) for every effective field theory of quantum gravity, with particles in arbitrary spin representations, was calculated.
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On the (A)dS decoupling limits of massive gravity

TL;DR: In this paper, the authors considered the decoupling of ghost-free massive gravity on (A)dS and showed a potential duality between this theory and a CFT on the boundary.
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Quantum de Sitter horizon entropy from quasicanonical bulk, edge, sphere and topological string partition functions

TL;DR: In this article , the exact one-loop corrected de Sitter entropy (the logarithm of the sphere partition function) for every effective field theory of quantum gravity, with particles in arbitrary spin representations, was calculated.
Posted Content

AdS one-loop partition functions from bulk and edge characters.

TL;DR: In this paper, it was shown that the one-loop partition function of any higher spin field in the anti-de-sitter space can be expressed as an integral transform of an O(2,d)-character and O( 2,d-2) edge character.
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Partition functions of p-forms from Harish-Chandra characters

TL;DR: In this article, the determinant of the co-exact p-form on spheres and anti-de Sitter spaces can be written as an integral transform of bulk and edge Harish-Chandra characters.
References
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BookDOI

The classical groups : their invariants and representations

Hermann Weyl
TL;DR: Weyl as discussed by the authors discusses the symmetric, full linear, orthogonal, and symplectic groups and determines their different invariants and representations using basic concepts from algebra, and examines the various properties of the groups.
Journal ArticleDOI

AdS dual of the critical O(N) vector model

TL;DR: In this article, a general relation between theories of infinite number of higher-spin massless gauge fields in AdS d + 1 and large N conformal theories in d dimensions containing N -component vector fields was proposed.
Journal ArticleDOI

Nonlinear equations for symmetric massless higher spin fields in (A)dSd

TL;DR: In this article, nonlinear field equations for totally symmetric bosonic massless fields of all spins in any dimension are presented, and a nonlinear nonlinear model of the field equations is proposed.
Journal ArticleDOI

Consistent equations for interacting gauge fields of all spins in 3+1 dimensions

TL;DR: In this paper, consistent equations of motion of interacting gauge fields of all spins in 3+1 dimensions are formulated in a closed form, which are explicitly general coordinate invariant, possess all necessary higher spin gauge symmetries and reduce to the usual equations of free massless fields at the linearized level.
Journal ArticleDOI

Massless higher spins and holography

TL;DR: A survey of massless HS theories with 32 supersymmetries in D =4,5,7 (where the 7D results are new) is given and corresponding composite operators are discussed in this paper.
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