Non-perturbative solutions for lattice quantum gravity
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The existence of this quantization ambiguity is due to the peculiar kind of representation on which nonperturbative quantum gravity is based.
“The existence of this quantization ambiguity is due to the peculiar kind of representation on which nonperturbative quantum gravity is based [5,6].”
From Immirzi parameter in quantum general relativity (1998) · cites this paper as [5]
This representation is characterized by the fact that the holonomy is a well-defined operator in the quantum theory.
“This representation is characterized by the fact that the holonomy is a well-defined operator in the quantum theory.”
From Immirzi parameter in quantum general relativity (1998) · cites this paper as [5]
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Self-citation
- Authors
- Loll, R.
- Affiliations
- Istituto Nazionale di Fisica Nucleare, Sezione di Firenze (IT)
- Corresponding author
- Loll, R.
- ORCID
- Loll, R.
- Venue
- Nuclear Physics B
- Publisher
- Elsevier BV
- Published
- 1995-06
- Volume
- 444
- Issue
- 3
- Pages
- 619-639
- ISSN
- 0550-3213 (ISSN-L)
- OpenAlex
- W2091923127
- Cited by
- 47
- References
- 28
- Citations by year
- 2012: 1
- FWCI
- 9.35
- Type
- journal article
- Language
- en
- Open access
- green
- arxiv.org
- Locations
- Nuclear Physics B (publishedVersion)
- arXiv (Cornell University) (submittedVersion)
- CERN Document Server (European Organization for Nuclear Research) (submittedVersion)
- Utrecht University Repository (Utrecht University) (submittedVersion, other-oa)
- arXiv (Cornell University)
- Topics
- Physical Sciences › Physics and Astronomy › Statistical and Nonlinear Physics › Noncommutative and Quantum Gravity Theories
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Relativity and Gravitational Theory
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Black Holes and Theoretical Physics
- Keywords
- lattice gravity, canonical quantum gravity, Wilson loops, Polyakov loop, Wheeler-DeWitt equation, non-perturbative solutions, gauge invariance, diffeomorphism invariance, kinematical Hilbert space, four-dimensional spacetime
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