Cited by 92Noncommutative and Quantum Gravity TheoriesAdvanced Operator Algebra ResearchRelativity and Gravitational Theory

Quantum groups and noncommutative geometry

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Majid, Shahn·2000·Journal of Mathematical Physics

Abstract

Quantum groups emerged in the latter quarter of the 20th century as, on the one hand, a deep and natural generalization of symmetry groups for certain integrable systems, and on the other as part of a generalization of geometry itself powerful enough to make sense in the quantum domain. Just as the last century saw the birth of classical geometry, so the present century sees at its end the birth of this quantum or noncommutative geometry, both as an elegant mathematical reality and in the form of the first theoretical predictions for Planck-scale physics via ongoing astronomical measurements. Noncommutativity of space–time, in particular, amounts to a postulated new force or physical effect called cogravity.

Integrity signals

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Crossref · 10.1063/1.533331

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79 of 79 references verified0 citation errors · 0 not checkable

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  • The Hilbert space of a quantum tetrahedron is the sum over all irreducible representations assigned to its triangles of all invariant tensors (intertwiners).

    “T = j i Inv(j 0 ⊗ j 1 ⊗ j 2 ⊗ j 3 ) (10 )”
  • For any group G, there is a category whose objects are non-degenerate spin networks and whose morphisms are non-degenerate spin foams.

    “It is important to note that, with these definitions of equivalence and composition we can define, for any given group G, a category F in which the objects are non-degenerate spin networks and the (non-degenerate) spin foams represent morphisms between them [13].”
  • The commutation relations of the quantum operators show that the four triangle area operators commute with each other and with the parallelogram area operators, among which only two are independent, while the parallelogram area operators have nonvanishing commutators among themselves.

    “Analysing the commutation relations of the quantum operators corresponding to the triangle and parallelogram area operators, it turns out (see [13,58]) that, while the four triangle area operators commute with each other and with the parallelogram areas operators (among which only two are independent), the last ones have nonvanishing commutators among themselves.”
  • The gluing procedure is consistent with the general spin foam formalism [13,14], which states that gluing two manifolds along a common boundary gives Z(M)Z(M')=Z(MM').

    “The gluing procedure used above is consistent with the formalism developed for general spin foams [13,14], and discussed in section 3, saying that, when we glue two manifolds M and M along a common boundary, the partition functions associated with them and with the composed manifold satisfy Z(M)Z(M ) = Z(MM )”

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Authors
Majid, S.
Affiliations
University of London (GB)
Corresponding author
Majid, Shahn
Venue
Journal of Mathematical Physics
Published
2000-06-01
Volume
41
Issue
6
Pages
3892-3942
ISSN
  • 0022-2488 (ISSN-L)
  • 1089-7658
OpenAlex
W2020855800
Cited by
92
References
79
Citations by year
2025: 2 · 2024: 5 · 2023: 4 · 2022: 1 · 2021: 6 · 2020: 3 · 2019: 1 · 2018: 3 · 2017: 3 · 2016: 2 · 2014: 2 · 2013: 3 · 2012: 6
FWCI
3.39
Type
journal article
Language
en
Open access
Locations
  • Journal of Mathematical Physics (publishedVersion)
  • arXiv (Cornell University) (submittedVersion)
  • CERN Document Server (European Organization for Nuclear Research) (submittedVersion)
  • arXiv (Cornell University)
Topics
  • Physical Sciences › Physics and Astronomy › Statistical and Nonlinear Physics › Noncommutative and Quantum Gravity Theories
  • Physical Sciences › Mathematics › Mathematical Physics › Advanced Operator Algebra Research
  • Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Relativity and Gravitational Theory
Keywords
quantum groups, noncommutative geometry, noncommutative spacetime, integrable systems, symmetry groups, Planck-scale physics, quantum geometry

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