Thermodynamic ensembles with cosmological horizons
Batoul Banihashemi, Ted Jacobson

TL;DR
This paper develops a rigorous statistical framework for de Sitter horizons by introducing a boundary in gravitational path integrals, analyzing thermodynamic phases, and connecting to the Gibbons-Hawking partition function.
Contribution
It introduces a boundary-based approach to define thermodynamic ensembles for de Sitter space, clarifying their statistical foundations and stability properties.
Findings
Formulation of path integrals over constrained phase space
Analysis of thermodynamic stability and phases
Derivation of Gibbons-Hawking partition function as a limit
Abstract
The entropy of a de Sitter horizon was derived long ago by Gibbons and Hawking via a gravitational partition function. Since there is no boundary at which to define the temperature or energy of the ensemble, the statistical foundation of their approach has remained obscure. To place the statistical ensemble on a firm footing we introduce an artificial "York boundary", with either canonical or microcanonical boundary conditions, as has been done previously for black hole ensembles. The partition function and the density of states are expressed as integrals over paths in the constrained, spherically reduced phase space of pure 3+1 dimensional gravity with a positive cosmological constant. Issues related to the domain and contour of integration are analyzed, and the adopted choices for those are justified as far as possible. The canonical ensemble includes a patch of spacetime without…
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