Abstract
In this chapter let us show that the irreducible parts ℬν, ℬ’ν (see VII § 5.4) permit a representation by Hilbert space operators, i.e. for ℬν, ℬ’ν there is a Hilbert space ℋν over the field R of real numbers or over the C of complex numbers or over the Q of quaternions where ℬν can be identified with the set of self-adjoint operators of the trace class and ℬ’ν with the set. of all bounded, self-adjoint operators, so that µ (x, y) = tr (x y). Then Kν is the set of all operators w ∈ ℬν with w ≧ 0, tr(w)= 1, while Lν is the set of all operators ɡ ∈ ℬ’ν with 0 ≦ɡ≦ 1
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© 1985 Springer-Verlag Berlin Heidelberg
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Ludwig, G. (1985). Representation of ℬ, ℬ’ by Banach Spaces of Operators in a Hilbert Space. In: An Axiomatic Basis for Quantum Mechanics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-70029-3_8
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DOI: https://doi.org/10.1007/978-3-642-70029-3_8
Publisher Name: Springer, Berlin, Heidelberg
Print ISBN: 978-3-642-70031-6
Online ISBN: 978-3-642-70029-3
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