An observer’s measure of de Sitter entropy

A bstract The two-point correlation function of a massive field ⟨ χ ( τ ) χ (0)⟩, measured along an observer’s worldline in de Sitter (dS), decays exponentially as τ → ∞. Meanwhile, every dS observer is surrounded by a horizon and the holographic interpretation of the horizon entropy S dS suggests that the correlation function should stop decaying, and start behaving erratically at late times. We find evidence for this expectation in Jackiw-Teitelboim gravity by finding a topologically nontrivial saddle, which is suppressed by $$ {e}^{-{S}_{\textrm{dS}}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mi>e</mml:mi> <mml:mrow> <mml:mo>−</mml:mo> <mml:msub> <mml:mi>S</mml:mi> <mml:mi>dS</mml:mi> </mml:msub> </mml:mrow> </mml:msup> </mml:math> , and which gives a constant contribution to | ⟨ χ ( τ ) χ (0)⟩ | 2 . This constant might have the interpretation of the late-time average of | ⟨ χ ( τ ) χ (0)⟩ | 2 over all microscopic theories that have the same low-energy effective description.

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Publication Details

Journal
Journal of High Energy Physics
Published
2024-10-09
DOI
https://doi.org/10.1007/jhep10(2024)077
Citations
6
Primary Topic
Black Holes and Theoretical Physics
Type
article
Field-Weighted Citation Impact
3.30

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article

An observer’s measure of de Sitter entropy

Mehrdad Mirbabayi
6 citations
Journal of High Energy Physics
Black Holes and Theoretical Physics
3.30
article

An observer’s measure of de Sitter entropy

Mehrdad Mirbabayi
article en
6 citations

Abstract

A bstract The two-point correlation function of a massive field ⟨ χ ( τ ) χ (0)⟩, measured along an observer’s worldline in de Sitter (dS), decays exponentially as τ → ∞. Meanwhile, every dS observer is surrounded by a horizon and the holographic interpretation of the horizon entropy S dS suggests that the correlation function should stop decaying, and start behaving erratically at late times. We find evidence for this expectation in Jackiw-Teitelboim gravity by finding a topologically nontrivial saddle, which is suppressed by $$ {e}^{-{S}_{\textrm{dS}}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mi>e</mml:mi> <mml:mrow> <mml:mo>−</mml:mo> <mml:msub> <mml:mi>S</mml:mi> <mml:mi>dS</mml:mi> </mml:msub> </mml:mrow> </mml:msup> </mml:math> , and which gives a constant contribution to | ⟨ χ ( τ ) χ (0)⟩ | 2 . This constant might have the interpretation of the late-time average of | ⟨ χ ( τ ) χ (0)⟩ | 2 over all microscopic theories that have the same low-energy effective description.

Journal of High Energy PhysicsVol. 2024(10)
The Abdus Salam International Centre for Theoretical Physics (ICTP) (IT)
CERN
Affordable and clean energy
Openalex Percentile: Top 6%
Black Holes and Theoretical Physics
3.30
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