Twisted reality and the second-order condition

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.

27 pages; no figures

References in corpus (3)

• Lorentz signature and twisted spectral triples
• Fermion masses, mass-mixing and the almost commutative geometry of the Standard Model
• On twisted reality conditions

Cited by in corpus (1)

• Gauge transformations of spectral triples with twisted real structures