2014
DOI: 10.1063/1.4898769
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On globally non-trivial almost-commutative manifolds

Abstract: Within the framework of Connes' noncommutative geometry, we define and study globally non-trivial (or topologically non-trivial) almost-commutative manifolds. In particular, we focus on those almostcommutative manifolds that lead to a description of a (classical) gauge theory on the underlying base manifold. Such an almost-commutative manifold is described in terms of a 'principal module', which we build from a principal fibre bundle and a finite spectral triple. We also define the purely algebraic notion of '… Show more

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Cited by 16 publications
(28 citation statements)
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“…As in [BD14], we construct almost-commutative manifolds as F × M instead of M × F (though the latter is more common in the literature). The reason is that the order F × M is more natural for the generalisation to the globally non-trivial case and its description as a Kasparov product (see [BD14, §III.C]).…”
Section: Almost-commutative Manifoldsmentioning
confidence: 99%
“…As in [BD14], we construct almost-commutative manifolds as F × M instead of M × F (though the latter is more common in the literature). The reason is that the order F × M is more natural for the generalisation to the globally non-trivial case and its description as a Kasparov product (see [BD14, §III.C]).…”
Section: Almost-commutative Manifoldsmentioning
confidence: 99%
“…that has the usual product form (7) though with a vanishing second term and acting not on the full tensor product of Hilbert spaces but only on its subspace.…”
Section: Second Isomorphic Spectral Triplementioning
confidence: 99%
“…So far we established isomorphisms between spectral triples by selecting Dirac operators, both for the first and second case, which act trivially as the identity on the finite part of the respective Hilbert spaces. In order to push further the analogy with almost commutative manifolds, hence with standard model of particles ([1], [7]), it would be interesting to get a Dirac operator whose action on the "internal" degrees of freedom is non trivial. In quantum field theory, internal degrees of freedom of a single, isolated fermion change whenever it moves in a space-time region with a gauge field (e.g.…”
Section: Curved Rational Noncommutative Torusmentioning
confidence: 99%
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