2016
DOI: 10.48550/arxiv.1601.07353
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Working with Nonassociative Geometry and Field Theory

Abstract: We review aspects of our formalism for differential geometry on noncommutative and nonassociative spaces which arise from cochain twist deformation quantization of manifolds. We work in the simplest setting of trivial vector bundles and flush out the details of our approach providing explicit expressions for all bimodule operations, and for connections and curvature. As applications, we describe the constructions of physically viable action functionals for Yang-Mills theory and Einstein-Cartan gravity on nonco… Show more

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Cited by 12 publications
(22 citation statements)
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“…This violation is well-known in twisted noncommutative differential geometry, see e.g. [1,9,16]. For trivial R-matrix, the right-hand sides of these covariant derivative equations vanish identically and we recover the usual Bianchi identity in classical geometry.…”
Section: Braided Curvaturementioning
confidence: 51%
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“…This violation is well-known in twisted noncommutative differential geometry, see e.g. [1,9,16]. For trivial R-matrix, the right-hand sides of these covariant derivative equations vanish identically and we recover the usual Bianchi identity in classical geometry.…”
Section: Braided Curvaturementioning
confidence: 51%
“…This paper arose as part of an ongoing programme to formulate a nonassociative theory of gravity that is inspired by scenarios in closed non-geometric string theory, see e.g. [9,16,18]. We argued in [28] that the L ∞ -algebra formalism should provide the natural receptacle to capture the failure of closure and covariance of field equations under nonassociative gauge transformations.…”
Section: Braided Noncommutative Gravitymentioning
confidence: 99%
“…This has led to attempts to treat noncommutative gravity as a deformation of a 'gauge theory', that is, in the first order formalism for general relativity: One uses the Einstein-Cartan principal bundle formulation, with star-gauge symmetry, where the corresponding variational principle is based on the Palatini action functional [10,22,34,37,41]. However, diffeomorphisms can never be implemented as star-gauge symmetries, in any formalism, and instead the noncommutative theory of gravity is invariant under a 'twisted' action of infinitesimal diffeomorphisms [16,19].…”
Section: Non-geometric Backgrounds and Noncommutative Gravitymentioning
confidence: 99%
“…the exterior algebra of differential forms on Ê 1,d−1 gives the noncommutative differential calculus discussed in Section 3.1; for the holonomic coframe L ∂ν dx µ = 0, so that indeed dx µ ∧ ⋆ dx ν = dx µ ∧ dx ν and λ ⋆ dx µ = dx µ ⋆ λ = λ • dx µ for λ ∈ Ω 0 (Ê 1,d−1 ). 22 Similarly, for the holonomic frame…”
Section: Drinfel'd Twist Deformation Theorymentioning
confidence: 99%
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