Dynamical edge modes in p-form gauge theories

A bstract We extend our recently identified dynamical edge mode boundary condition to p -form gauge theories, revealing their edge modes as Goldstone bosons arising from gauge transformations with support on the boundary. The symplectic conjugates of these edge modes correspond to the electric-field-like components normal to the boundary. We demonstrate that both the symplectic form and the Hamiltonian naturally decompose into bulk and edge parts. When the boundary is a stretched horizon, we show that the thermal edge partition function reduces to that of a codimension-two ghost ( p – 1)-form residing on the bifurcation surface. These findings provide a dynamical framework that elucidates observations made by several authors. Additionally, we generalize Donnelly and Wall’s non-dynamical approach to obtain edge partition functions for both massive and massless p -forms. In the context of a de Sitter static patch, these results are consistent with the edge partition functions found by several authors in arbitrary dimensions.

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Publication Details

Journal
Journal of High Energy Physics
Published
2025-02-26
DOI
https://doi.org/10.1007/jhep02(2025)182
Citations
3
Primary Topic
Black Holes and Theoretical Physics
Type
article
Field-Weighted Citation Impact
5.61
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article

Dynamical edge modes in p-form gauge theories

Adam Ball, Y. T. Albert Law
3 citations
Journal of High Energy Physics
Black Holes and Theoretical Physics
5.61
article

Dynamical edge modes in p-form gauge theories

Adam Ball, Y. T. Albert Law
article en
3 citations

Abstract

A bstract We extend our recently identified dynamical edge mode boundary condition to p -form gauge theories, revealing their edge modes as Goldstone bosons arising from gauge transformations with support on the boundary. The symplectic conjugates of these edge modes correspond to the electric-field-like components normal to the boundary. We demonstrate that both the symplectic form and the Hamiltonian naturally decompose into bulk and edge parts. When the boundary is a stretched horizon, we show that the thermal edge partition function reduces to that of a codimension-two ghost ( p – 1)-form residing on the bifurcation surface. These findings provide a dynamical framework that elucidates observations made by several authors. Additionally, we generalize Donnelly and Wall’s non-dynamical approach to obtain edge partition functions for both massive and massless p -forms. In the context of a de Sitter static patch, these results are consistent with the edge partition functions found by several authors in arbitrary dimensions.

Journal of High Energy PhysicsVol. 2025(2)
Perimeter Institute (CA), Instituto de Física Teórica (ES)
Openalex Percentile: Top 6%
Black Holes and Theoretical Physics
5.61
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