Galina, E.; Kaplan, A.; Saal, L. Charged representations of the infinite Fermi and Clifford algebras. (English) Zbl 1115.81039 Lett. Math. Phys. 72, No. 1, 65-77 (2005). Summary: The real and quaternionic charge conjugation operators invariant under the infinite-dimensional Clifford algebra, or compatible with the Fermi algebra, are determined. There results a maze of inequivalent irreducible charged representations, all of which are non-Fock. The representation vectors and their charges admit two interpretations besides those of spinors or states of quantum fields: as wavelets on the circle, with charge conjugations acting via ordinary complex conjugation; and as infinite-dimensional numbers, with charge conjugations acting by automorphisms. MSC: 81R15 Operator algebra methods applied to problems in quantum theory 15A66 Clifford algebras, spinors 46N50 Applications of functional analysis in quantum physics 81R10 Infinite-dimensional groups and algebras motivated by physics, including Virasoro, Kac-Moody, \(W\)-algebras and other current algebras and their representations Keywords:spinors; CAR algebra; non-Fock representations PDF BibTeX XML Cite \textit{E. Galina} et al., Lett. Math. Phys. 72, No. 1, 65--77 (2005; Zbl 1115.81039) Full Text: DOI References: [5] Guichardet, A. (1968). In: A. Colin (ed.). Algèbres d’observables Associées aux Relations de Commutation. · Zbl 0169.17302 [7] Galina, E., Kaplan, A. and Saal, L.: Split Clifford modules over a Hilbert space, Math. RT/0204117 (2002), 1–11. [9] Kadison, R., Ringrose, J. (1969). Fundamentals of the theory of operator algebras. Amer. Math. Soc. Ed.: 1998. · Zbl 0601.46054 [11] Lawson, H., Michelsohn, M. (1989). Spin Geometry, Princeton University Press, 1989. · Zbl 0688.57001 This reference list is based on information provided by the publisher or from digital mathematics libraries. Its items are heuristically matched to zbMATH identifiers and may contain data conversion errors. It attempts to reflect the references listed in the original paper as accurately as possible without claiming the completeness or perfect precision of the matching.