Gradient flow of Einstein-Maxwell theory and Reissner-Nordström black holes

Abstract Ricci flow is a natural gradient flow of the Einstein-Hilbert action. Here we consider the analog for the Einstein-Maxwell action, which gives Ricci flow with a stress tensor contribution coupled to a Yang-Mills flow for the Maxwell field. We argue that this flow is well-posed for static sp...

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Main Authors: Davide De Biasio, Julian Freigang, Dieter Lüst, Toby Wiseman
Format: Article
Language:English
Published: SpringerOpen 2023-03-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP03(2023)074
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author Davide De Biasio
Julian Freigang
Dieter Lüst
Toby Wiseman
author_facet Davide De Biasio
Julian Freigang
Dieter Lüst
Toby Wiseman
author_sort Davide De Biasio
collection DOAJ
description Abstract Ricci flow is a natural gradient flow of the Einstein-Hilbert action. Here we consider the analog for the Einstein-Maxwell action, which gives Ricci flow with a stress tensor contribution coupled to a Yang-Mills flow for the Maxwell field. We argue that this flow is well-posed for static spacetimes with pure electric or magnetic potentials and show it preserves both non-extremal and extremal black hole horizons. In the latter case we find the flow of the near horizon geometry decouples from that of the exterior. The Schwarzschild black hole is an unstable fixed point of Ricci flow for static spacetimes. Here we consider flows of the Reissner-Nordström (RN) fixed point. The magnetic RN solution becomes a stable fixed point of the flow for sufficient charge. However we find that the electric RN black hole is always unstable. Numerically solving the flow starting with a spherically symmetric perturbation of a non-extremal RN solution, we find similar behaviour in the electric case to the Ricci flows of perturbed Schwarzschild, namely the horizon shrinks to a singularity in finite time or expands forever. In the magnetic case, a perturbed unstable RN solution has a similar expanding behaviour, but a perturbation that decreases the horizon size flows to a stable black hole solution rather than a singularity. For extremal RN we solve the near horizon flow for spherical symmetry exactly, and see in the electric case two unstable directions which flow to singularities in finite flow time. However, even turning these off, and fixing the near horizon geometry to be that of RN, we numerically show that the flows appear to become singular in the vicinity of its horizon.
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spelling doaj.art-8709851cb72a43af8eb4f751fcbffa6c2023-06-25T11:06:47ZengSpringerOpenJournal of High Energy Physics1029-84792023-03-012023315110.1007/JHEP03(2023)074Gradient flow of Einstein-Maxwell theory and Reissner-Nordström black holesDavide De Biasio0Julian Freigang1Dieter Lüst2Toby Wiseman3Max-Planck-Institut für Physik, Werner-Heisenberg-InstitutMax-Planck-Institut für Physik, Werner-Heisenberg-InstitutMax-Planck-Institut für Physik, Werner-Heisenberg-InstitutTheoretical Physics Group, Blackett Laboratory, Imperial College LondonAbstract Ricci flow is a natural gradient flow of the Einstein-Hilbert action. Here we consider the analog for the Einstein-Maxwell action, which gives Ricci flow with a stress tensor contribution coupled to a Yang-Mills flow for the Maxwell field. We argue that this flow is well-posed for static spacetimes with pure electric or magnetic potentials and show it preserves both non-extremal and extremal black hole horizons. In the latter case we find the flow of the near horizon geometry decouples from that of the exterior. The Schwarzschild black hole is an unstable fixed point of Ricci flow for static spacetimes. Here we consider flows of the Reissner-Nordström (RN) fixed point. The magnetic RN solution becomes a stable fixed point of the flow for sufficient charge. However we find that the electric RN black hole is always unstable. Numerically solving the flow starting with a spherically symmetric perturbation of a non-extremal RN solution, we find similar behaviour in the electric case to the Ricci flows of perturbed Schwarzschild, namely the horizon shrinks to a singularity in finite time or expands forever. In the magnetic case, a perturbed unstable RN solution has a similar expanding behaviour, but a perturbation that decreases the horizon size flows to a stable black hole solution rather than a singularity. For extremal RN we solve the near horizon flow for spherical symmetry exactly, and see in the electric case two unstable directions which flow to singularities in finite flow time. However, even turning these off, and fixing the near horizon geometry to be that of RN, we numerically show that the flows appear to become singular in the vicinity of its horizon.https://doi.org/10.1007/JHEP03(2023)074Black HolesBlack Holes in String TheoryClassical Theories of GravityModels of Quantum Gravity
spellingShingle Davide De Biasio
Julian Freigang
Dieter Lüst
Toby Wiseman
Gradient flow of Einstein-Maxwell theory and Reissner-Nordström black holes
Journal of High Energy Physics
Black Holes
Black Holes in String Theory
Classical Theories of Gravity
Models of Quantum Gravity
title Gradient flow of Einstein-Maxwell theory and Reissner-Nordström black holes
title_full Gradient flow of Einstein-Maxwell theory and Reissner-Nordström black holes
title_fullStr Gradient flow of Einstein-Maxwell theory and Reissner-Nordström black holes
title_full_unstemmed Gradient flow of Einstein-Maxwell theory and Reissner-Nordström black holes
title_short Gradient flow of Einstein-Maxwell theory and Reissner-Nordström black holes
title_sort gradient flow of einstein maxwell theory and reissner nordstrom black holes
topic Black Holes
Black Holes in String Theory
Classical Theories of Gravity
Models of Quantum Gravity
url https://doi.org/10.1007/JHEP03(2023)074
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