1968
DOI: 10.1119/1.1975143
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Foundations of Quantum Mechanics

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Cited by 306 publications
(435 citation statements)
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“…In the sixties and seventies, new formalisms were being investigated by many research groups. In Geneva, the school of Josef Maria Jauch was developing an axiomatic formulation of quantum mechanics [20], and Constantin Piron gave the proof of a fundamental representation theorem for the axiomatic structure [21]. Gunther Ludwig's group in Marburg [22] developed the convex ensemble theory, and in Amherst, Massachusetts, the group of Charles Randall and David Foulis [23,24] was elaborating an operational approach.…”
Section: Magic With Neutronsmentioning
confidence: 99%
“…In the sixties and seventies, new formalisms were being investigated by many research groups. In Geneva, the school of Josef Maria Jauch was developing an axiomatic formulation of quantum mechanics [20], and Constantin Piron gave the proof of a fundamental representation theorem for the axiomatic structure [21]. Gunther Ludwig's group in Marburg [22] developed the convex ensemble theory, and in Amherst, Massachusetts, the group of Charles Randall and David Foulis [23,24] was elaborating an operational approach.…”
Section: Magic With Neutronsmentioning
confidence: 99%
“…As regards the main requirements of a satisfactory theory of the measurement process, it is clear from the works of Bohr [8], Jauch [9] and Van Kampen [2] that such a theory demands both a characterisation of the macroscopicality of the observables M and an amplification property of the S − I coupling whereby different microstates of S give rise to macroscopically different states of I. Evidently, this implies that the initial state in which I is prepared must be unstable against microscopic changes in the state of S. On the other hand, as emphasised by Whitten-Wolfe and Emch [10,11], the correspondence between the microstate of S and the eventual observed macrostate of I must be stable against macroscopically small changes in the initial state of this instrument, of the kind that are inevitable in experimental procedures. Thus, the initial state of I must be metastable by virtue of this combination of stability and instability properties.…”
Section: Introductory Discussionmentioning
confidence: 99%
“…Our treatment of this model is designed to obtain conditions on the S − I coupling that lead to both the reduction of the wave-packet and the required correspondence between the reading of the instrument's pointer and the resultant state of S. As in the works [2] , [8][9][10][11] and [14], we avoid the assumption of Von Neumann [1] and Wigner [19] that the observation of the pointer of I requires another measuring instrument, I 2 , which in turn requires yet another instrument, and so on, in such a way that the whole process involves an infinite regression ending up in the observer's brain! Instead, we assume that the measurement process ends with the reading of the pointers that evaluate the macrovariables M of I.…”
Section: Introductory Discussionmentioning
confidence: 99%
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“…This has been the case, most prominently, in [29,39,40] and also in an important state-of-the-art book [4]. Quantum logical assumptions are simple enough to be accessible for direct comprehension, in contrast to Mackey's mathematically formulated axioms, but they tend to be linguistic rather than physical.…”
Section: M9mentioning
confidence: 99%