The DOI matches its Crossref record; 8 of the 8 references it cites were found in a registry or an index.
Quantum extension of the Kruskal spacetime
Open accessAbstract
A new description of macroscopic Kruskal black holes that incorporates the quantum geometry corrections of loop quantum gravity is presented. It encompasses both the `interior' region that contains classical singularities and the `exterior' asymptotic region. Singularities are naturally resolved by the quantum geometry effects of loop quantum gravity. The resulting quantum extension of space-time has the following features: (i) It admits an infinite number of trapped, anti-trapped and asymptotic regions; (ii) All curvature scalars have uniform (i.e., mass independent) upper bounds; (iii) In the large mass limit, all asymptotic regions of the extension have the same ADM mass; (iv) In the low curvature region (e.g., near horizons) quantum effects are negligible, as one would physically expect; and (v) Final results are insensitive to the fiducial structures that have to be introduced to construct the classical phase space description (as they must be). Previous effective theories [1-10] shared some but not all of these features. We compare and contrast our results with those of these effective theories and also with expectations based on the AdS/CFT conjecture [11]. We conclude with a discussion of limitations of our framework, especially for the analysis of evaporating black holes.
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Cites
Particle creation by black holes
Hawking, S. W. (1975) · Communications In Mathematical Physics · doi:10.1007/bf02345020 · Cited by 13,106 · cited 2×
“For example, in the commonly used Penrose diagram of an evaporating black hole –first introduced by Hawking [42] over 40 years ago– a singularity constitutes part of the future boundary of space-time even after the black hole has completely disappeared.”
Quantum nature of the big bang: Improved dynamics
Ashtekar, A., Pawlowski, T., & Singh, P. (2006) · Physical Review D · doi:10.1103/physrevd.74.084003 · Cited by 1,147 · cited 6×
“In FLRW models, limitations of the μo scheme were overcome through the so-called μ̄ scheme [22].”
InfluentialSelf-citationMathematical structure of loop quantum cosmology
Ashtekar, A., Bojowald, M., & Lewandowski, J. (2003) · Advances in Theoretical and Mathematical Physics · doi:10.4310/atmp.2003.v7.n2.a2 · Cited by 762
Self-citationQuantum nature of the big bang: An analytical and numerical investigation
Ashtekar, A., Pawlowski, T., & Singh, P. (2006) · Physical Review D · doi:10.1103/physrevd.73.124038 · Cited by 609
Self-citationUniqueness of Diffeomorphism Invariant States on Holonomy–Flux Algebras
Lewandowski, J., Okołów, A., Sahlmann, H., & Thiemann, T. (2006) · Communications in Mathematical Physics · doi:10.1007/s00220-006-0100-7 · Cited by 297
Taveras, V. (2008) · Physical Review D · doi:10.1103/physrevd.78.064072 · Cited by 280
Representations of the Weyl Algebra in Quantum Geometry
Fleischhack, C. (2009) · Communications in Mathematical Physics · doi:10.1007/s00220-008-0593-3 · Cited by 183
Is loop quantization in cosmology unique?
Corichi, A., & Singh, P. (2008) · Physical Review D · doi:10.1103/physrevd.78.024034 · Cited by 134
Self-citation
Cited by
Quantum Transfiguration of Kruskal Black Holes
Ashtekar, A., Olmedo, J., & Singh, P. (2018) · Physical Review Letters · doi:10.1103/physrevlett.121.241301 · Cited by 284
Self-citationBlack holes, white holes, and near-horizon physics
Gaur, R., & Visser, M. (2024) · Journal of High Energy Physics · doi:10.1007/jhep05(2024)172 · Cited by 11
Metadata
- Authors
- Ashtekar, A., Olmedo, J., & Singh, P.
- Venue
- Physical Review D
- Publisher
- American Physical Society (APS)
- Published
- 2018-12-10
- Volume
- 98
- Issue
- 12
- ISSN
- 2470-0010 (ISSN-L)
- 2470-0029
- OpenAlex
- W2806360372
- Cited by
- 239
- References
- 8
- FWCI
- 11.92
- Type
- journal article
- Language
- en
- Open access
- green
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