The (No) Boundary Proposal and excited states in de Sitter holography
Marcelo Botta-Cantcheff, Facundo Lorenzo Cruz, Pedro J. Martinez

TL;DR
This paper explores the extension of the no boundary proposal in de Sitter holography to include excited states by adding boundaries and boundary conditions, affecting late-time cosmological observables and advancing the holographic dictionary.
Contribution
It introduces a method to define excited states in de Sitter holography through boundary conditions, expanding the no boundary proposal beyond the ground state.
Findings
Consistent computation of n-point functions with excited states.
Late-time observables are modified in these excited states.
Potential implications for the holographic dictionary in de Sitter space.
Abstract
In the AdS/CFT framework, vacuum and excited states are systematically described by imposing arbitrary Dirichlet boundary conditions at the AdS boundary. Furthermore, there are explicit relations connecting the quantum states to their corresponding dual Euclidean AdS geometries, in line with the Hartle-Hawking (HH) construction. The ground state therefore corresponds to the dominant saddle point under trivial conditions on the asymptotic boundary, which is the exact Euclidean AdS geometry. In contrast, the situation in de Sitter spacetime differs significantly, as there is no natural region analogous to the AdS boundary. Thus, the Hartle Hawking approach precisely defines the ground state as a path integral over smooth (Euclidean) geometries ending on a spatial Cauchy surface, with \textit{no} additional boundary or past singularity, known as the no boundary proposal. In this work, we…
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Taxonomy
TopicsBlack Holes and Theoretical Physics · Noncommutative and Quantum Gravity Theories · Quantum Electrodynamics and Casimir Effect
