An interesting feature of the finite-dimensional real spectral triple (A, H, D, J) of the Standard Model is that it satisfies a "second-order" condition: conjugation by J maps the Clifford algebra Cl-D (A) into its commutant, which in fact is isomorphic to the Clifford algebra itself (H is a self-Morita equivalence Cl-D (A)-bimodule). This resembles a property of the canonical spectral triple of a closed oriented Riemannian manifold: there is a dense subspace of H which is a self-Morita equivalence Cl-D (A)-bimodule. In this paper we argue that on manifolds, in order for the self-Morita equivalence to be implemented by a reality operator J, one has to introduce a "twist" and weaken one of the axioms of real spectral triples. We then investigate how the above mentioned conditions behave under products of spectral triples.
Twisted Reality and the Second-Order Condition / Dabrowski, L.; D'Andrea, F.; Magee, A. M.. - In: MATHEMATICAL PHYSICS ANALYSIS AND GEOMETRY. - ISSN 1385-0172. - 24:2(2021), pp. 1-27. [10.1007/s11040-021-09384-4]
Twisted Reality and the Second-Order Condition
Dabrowski, L.;Magee, A. M.
2021-01-01
Abstract
An interesting feature of the finite-dimensional real spectral triple (A, H, D, J) of the Standard Model is that it satisfies a "second-order" condition: conjugation by J maps the Clifford algebra Cl-D (A) into its commutant, which in fact is isomorphic to the Clifford algebra itself (H is a self-Morita equivalence Cl-D (A)-bimodule). This resembles a property of the canonical spectral triple of a closed oriented Riemannian manifold: there is a dense subspace of H which is a self-Morita equivalence Cl-D (A)-bimodule. In this paper we argue that on manifolds, in order for the self-Morita equivalence to be implemented by a reality operator J, one has to introduce a "twist" and weaken one of the axioms of real spectral triples. We then investigate how the above mentioned conditions behave under products of spectral triples.File | Dimensione | Formato | |
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