Abstract
A consistent variational procedure applied to the gravitational action requires according to Gibbons and Hawking a certain balance between the volume and boundary parts of the action. We consider the problem of preserving this balance in the quantum effective action for the matter non-minimally coupled to metric. It is shown that one has to add a special boundary term to the matter action analogous to the Gibbons-Hawking one. This boundary term modifies the one-loop quantum corrections to give a correct balance for the effective action as well. This means that the boundary UV divergences do not require independent renormalization and are automatically renormalized simultaneously with their volume part. This result is derived for arbitrary non-minimally coupled matter. The example of 2D Maxwell field is considered in much detail. The relevance of the results obtained to the problem of the renormalization of the black hole entropy is discussed.
Full Text
Topics from this Paper
Non-minimally Coupled
Boundary Term
Black Hole Entropy
Effective Action
Special Term
+ Show 5 more
Create a personalized feed of these topics
Get StartedTalk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Similar Papers
Nuclear Physics
Nov 11, 1996
arXiv: General Relativity and Quantum Cosmology
Dec 28, 1995
Physical Review D
Mar 17, 2014
Physical Review D
Aug 31, 2022
arXiv: General Relativity and Quantum Cosmology
May 21, 2003
Physical Review D
May 3, 2016
Physical Review D
Nov 19, 2021
arXiv: High Energy Physics - Theory
May 16, 2012
arXiv: High Energy Physics - Theory
May 28, 2004
Classical and Quantum Gravity
Oct 21, 2003
arXiv: High Energy Physics - Theory
May 7, 2001
Physical Review D
Oct 15, 2015
Physics of the Dark Universe
Mar 1, 2022
Journal of Cosmology and Astroparticle Physics
Apr 1, 2018
Journal of Cosmology and Astroparticle Physics
Feb 26, 2018
Nuclear Physics B
Nuclear Physics B
Dec 1, 2023
Nuclear Physics B
Dec 1, 2023
Nuclear Physics B
Nov 1, 2023
Nuclear Physics B
Nov 1, 2023
Nuclear Physics B
Nov 1, 2023
Nuclear Physics B
Nov 1, 2023
Nuclear Physics B
Nov 1, 2023
Nuclear Physics B
Nov 1, 2023
Nuclear Physics B
Nov 1, 2023
Nuclear Physics B
Nov 1, 2023