Static Spherically Symmetric Black Holes in Weak <i>f</i>(<i>T</i>)-Gravity

With the advent of gravitational wave astronomy and first pictures of the “shadow” of the central black hole of our milky way, theoretical analyses of black holes (and compact objects mimicking them sufficiently closely) have become more important than ever. The near future promises more and more de...

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Main Authors: Christian Pfeifer, Sebastian Schuster
Format: Article
Language:English
Published: MDPI AG 2021-05-01
Series:Universe
Subjects:
Online Access:https://www.mdpi.com/2218-1997/7/5/153
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author Christian Pfeifer
Sebastian Schuster
author_facet Christian Pfeifer
Sebastian Schuster
author_sort Christian Pfeifer
collection DOAJ
description With the advent of gravitational wave astronomy and first pictures of the “shadow” of the central black hole of our milky way, theoretical analyses of black holes (and compact objects mimicking them sufficiently closely) have become more important than ever. The near future promises more and more detailed information about the observable black holes and black hole candidates. This information could lead to important advances on constraints on or evidence for modifications of general relativity. More precisely, we are studying the influence of weak teleparallel perturbations on general relativistic vacuum spacetime geometries in spherical symmetry. We find the most general family of spherically symmetric, static vacuum solutions of the theory, which are candidates for describing teleparallel black holes which emerge as perturbations to the Schwarzschild black hole. We compare our findings to results on black hole or static, spherically symmetric solutions in teleparallel gravity discussed in the literature, by comparing the predictions for classical observables such as the photon sphere, the perihelion shift, the light deflection, and the Shapiro delay. On the basis of these observables, we demonstrate that among the solutions we found, there exist spacetime geometries that lead to much weaker bounds on teleparallel gravity than those found earlier. Finally, we move on to a discussion of how the teleparallel perturbations influence the Hawking evaporation in these spacetimes.
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spelling doaj.art-07bd5c0897b545b3b77322c5a6c1f1672023-11-21T20:09:01ZengMDPI AGUniverse2218-19972021-05-017515310.3390/universe7050153Static Spherically Symmetric Black Holes in Weak <i>f</i>(<i>T</i>)-GravityChristian Pfeifer0Sebastian Schuster1Center of Applied Space Technology and Microgravity—ZARM, University of Bremen, Am Fallturm 2, 28359 Bremen, GermanyÚstav Teoretické Fyziky, Matematicko-Fyzikální Fakulta, Univerzita Karlova, V Holešovičkách 2, 180 00 Praha 8, Czech RepublicWith the advent of gravitational wave astronomy and first pictures of the “shadow” of the central black hole of our milky way, theoretical analyses of black holes (and compact objects mimicking them sufficiently closely) have become more important than ever. The near future promises more and more detailed information about the observable black holes and black hole candidates. This information could lead to important advances on constraints on or evidence for modifications of general relativity. More precisely, we are studying the influence of weak teleparallel perturbations on general relativistic vacuum spacetime geometries in spherical symmetry. We find the most general family of spherically symmetric, static vacuum solutions of the theory, which are candidates for describing teleparallel black holes which emerge as perturbations to the Schwarzschild black hole. We compare our findings to results on black hole or static, spherically symmetric solutions in teleparallel gravity discussed in the literature, by comparing the predictions for classical observables such as the photon sphere, the perihelion shift, the light deflection, and the Shapiro delay. On the basis of these observables, we demonstrate that among the solutions we found, there exist spacetime geometries that lead to much weaker bounds on teleparallel gravity than those found earlier. Finally, we move on to a discussion of how the teleparallel perturbations influence the Hawking evaporation in these spacetimes.https://www.mdpi.com/2218-1997/7/5/153teleparallel gravityblack holeshorizonBirkhoff theoremphoton sphereShapiro delay
spellingShingle Christian Pfeifer
Sebastian Schuster
Static Spherically Symmetric Black Holes in Weak <i>f</i>(<i>T</i>)-Gravity
Universe
teleparallel gravity
black holes
horizon
Birkhoff theorem
photon sphere
Shapiro delay
title Static Spherically Symmetric Black Holes in Weak <i>f</i>(<i>T</i>)-Gravity
title_full Static Spherically Symmetric Black Holes in Weak <i>f</i>(<i>T</i>)-Gravity
title_fullStr Static Spherically Symmetric Black Holes in Weak <i>f</i>(<i>T</i>)-Gravity
title_full_unstemmed Static Spherically Symmetric Black Holes in Weak <i>f</i>(<i>T</i>)-Gravity
title_short Static Spherically Symmetric Black Holes in Weak <i>f</i>(<i>T</i>)-Gravity
title_sort static spherically symmetric black holes in weak i f i i t i gravity
topic teleparallel gravity
black holes
horizon
Birkhoff theorem
photon sphere
Shapiro delay
url https://www.mdpi.com/2218-1997/7/5/153
work_keys_str_mv AT christianpfeifer staticsphericallysymmetricblackholesinweakifiitigravity
AT sebastianschuster staticsphericallysymmetricblackholesinweakifiitigravity