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The geometry of the state space

In A. R. Marlow (ed.), Mathematical foundations of quantum theory. New York: Academic Press. pp. 153--176 (1978)

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  1. Observables on hypergraphs.S. P. Gudder & G. T. Rüttimann - 1986 - Foundations of Physics 16 (8):773-790.
    Observables on hypergraphs are described by event-valued measures. We first distinguish between finitely additive observables and countably additive ones. We then study the spectrum, compatibility, and functions of observables. Next a relationship between observables and certain functionals on the set of measures M(H) of a hypergraph H is established. We characterize hypergraphs for which every linear functional on M(H) is determined by an observable. We define the concept of an “effect” and show that observables are related to effect-valued measures. Finally, (...)
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  • Semantics in Banach spaces.Sławomir Bugajski - 1983 - Studia Logica 42 (1):81 - 88.
    A new approach to semantics, based on ordered Banach spaces, is proposed. The Banach spaces semantics arises as a generalization of the four particular cases: the Giles' approach to belief structures, its generalization to the non-Boolean case, and fuzzy extensions of Boolean as well as of non-Boolean semantics.
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  • Semantics in Banach spaces.S.?Awomir Bugajski - 1983 - Studia Logica 42 (1):81-88.
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  • Realism, operationalism, and quantum mechanics.D. Foulis, C. Piron & C. Randall - 1983 - Foundations of Physics 13 (8):813-841.
    A comprehensive formal system is developed that amalgamates the operational and the realistic approaches to quantum mechanics. In this formalism, for example, a sharp distinction is made between events, operational propositions, and the properties of physical systems.
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  • Logical foundations of modern cybernetics.A. Szymanski & J. M. Szymanski - 1995 - World Futures 44 (2):177-180.
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  • Weak density of states.Gottfried T. Rüttimann - 1989 - Foundations of Physics 19 (9):1101-1112.
    Let L be a quantum logic, here an orthoalgebra, and let Δ be a convex set of states on L. Then Δ generates a base-normed space, and the dual-order unit-normed space contains a canonically constructed homomorphic copy of L, denoted by eΔ(L). A convex set Δ of states on L is said to be ample provided that every state on L is obtained by restricting an element of the base of the bi-dual order unit-normed space to eΔ(L). For a quantum (...)
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