By Breit G.
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Extra resources for An Interpretation of Diracs Theory of the Electron
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Moreover, we get that ςN (M1 β ∗γ M2 ) = M2 γ ∗β M1 . In particular, we have No N (M1 ∩ β(N ) ) β ⊗γ (M2 ∩ γ (N) ) ⊂ M1 β ∗γ M2 N N and M1 β ∗γ γ (N ) = (M1 ∩ β(N) ) β ⊗γ 1. N N 26 Michel Enock More generally, if β is a non-degenerate normal involutive anti-homomorphism from N into a von Neumann algebra M1 , and γ a non-degenerate normal involutive homomorphism from N into a von Neumann algebra M2 , it is possible to define, without any reference to a specific Hilbert space, a von Neumann algebra M1 β ∗γ M2 .
Q ; q)n (1) a a ; q, z = (b; q)∞ 1 ϕ1 ; q, z . See  for an b b extensive treatment on q-hypergeometric functions. The analysis of the dual of quantum SU(1, 1) depends heavily on Al-Salam & Chihara polynomials and little q-Jacobi functions.