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Foundations of Physics

On compatibility in quantum logics

Jiří Brabec, Pavel Pt�k

Published Feb 1, 1982• 19 citations
Publisher
DOI
10.1007/bf00736849

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It is shown that for any quantum logic LLL one can find a concrete logic KKK and a surjective homomorphism fff from KKK onto LLL such that fff maps the centre of KKK onto the centre of LLL. Moreover, one can ensure that each finite set of compatible elements in LLL is the image of a compatible subset of KKK. This result is "best possible" - let a logic LLL be the homomorphic image of a concrete logic under a homomorphism such that, if FFF is a finite subset of the pre-image of a compatible subset of LLL, then FFF is compatible. Then LLL must be concrete. In the second part one considers embeddings into concrete logics. It is shown that any concrete logic can be embedded into a concrete logic with preassigned centre and an abundance of two-valued measures. Finally, one proves that an arbitrary logic can be mapped into a concrete logic by a centrally additive mapping which preserves the ordering and complementation.
We consider the standard quantum logic L(H){\mathcal L}(H)L(H) associated to a complex Hilbert space HHH, i.e. the lattice of closed subspaces of HHH together with the orthogonal complementation. The orthogonality and compatibility relations are defined for any logic. In the standard quantum logic, they have a simple interpretation in terms of operator theory. For example, two closed subspaces (propositions in the logic L(H){\mathcal L}(H)L(H)) are compatible if and only if the projections on these subspaces commute. We present both classical and more resent results on transformations of L(H){\mathcal L}(H)L(H) and the associated Grassmannians which preserve the orthogonality or compatibility relation. The first result in this direction was classical Wigner's theorem.
The notion of a joint distribution in σ\sigmaσ-finite measures of observables of a quantum logic defined on some system of σ\sigmaσ-independent Boolean sub-σ\sigmaσ-algebras of a Boolean σ\sigmaσ-algebra is studied. In the present first part of the paper the author studies a joint distribution of compatible observables. It is shown that it may exists, although a joint obsevable of compatible observables need not exist.