Gauge dynamics in the C-representation
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The A = -1 Kauffman bracket of a spin network is the same as Penrose's spin network evaluation.
“Thus, the A = -1 Kauffman bracket of a spin network is the same at the Penrose's spin network evaluation.”
From Geometry eigenvalues and the scalar product from recoupling theory in loop quantum gravity (1996) · cites this paper as [46]
Cites
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Quantum chromodynamics as dynamics of loops
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Spin networks and quantum gravity
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Linking topological quantum field theory and nonperturbative quantum gravity
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The physical Hamiltonian in nonperturbative quantum gravity
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Causal evolution of spin networks
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Self-citationQuantum spin dynamics: VIII. The master constraint
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- Authors
- Gambini, R., & Trias, A.
- Affiliations
- Universitat Autònoma de Barcelona (ES)
- ORCID
- Gambini, Rodolfo
- Venue
- Nuclear Physics B
- Publisher
- Elsevier BV
- Published
- 1986-12
- Volume
- 278
- Issue
- 2
- Pages
- 436-448
- ISSN
- 0550-3213 (ISSN-L)
- OpenAlex
- W2086900751
- Cited by
- 130
- References
- 12
- Citations by year
- 2025: 1 · 2023: 1 · 2022: 2 · 2021: 2 · 2018: 1 · 2017: 1 · 2016: 1 · 2015: 3 · 2014: 1 · 2012: 2
- FWCI
- 1.10
- Type
- journal article
- Language
- en
- Open access
- closed
- Locations
- Nuclear Physics B (publishedVersion)
- Topics
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Quantum Chromodynamics and Particle Interactions
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Particle physics theoretical and experimental studies
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum and Classical Electrodynamics
- Keywords
- gauge theory, Hamiltonian dynamics, non-perturbative formulation
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