Author:
García-Quismondo Alejandro,Mena Marugán Guillermo A.
Abstract
In this article, we reexamine the derivation of the dynamical equations of the Ashtekar-Olmedo-Singh black hole model in order to determine whether it is possible to construct a Hamiltonian formalism where the parameters that regulate the introduction of quantum geometry effects are treated as true constants of motion. After arguing that these parameters should capture contributions from two distinct sectors of the phase space that had been considered independent in previous analyses in the literature, we proceed to obtain the corresponding equations of motion and analyze the consequences of this more general choice. We restrict our discussion exclusively to these dynamical issues. We also investigate whether the proposed procedure can be reconciled with the results of Ashtekar, Olmedo, and Singh, at least in some appropriate limit.
Funder
Ministerio de Ciencia e Innovación
Fundación Bancaria Caixa d'Estalvis i Pensions de Barcelona
Subject
Astronomy and Astrophysics
Cited by
14 articles.
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