1983
DOI: 10.1007/978-3-642-86751-4
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Foundations of Quantum Mechanics I

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Cited by 430 publications
(409 citation statements)
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“…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. Peter Mittelstaedt and his group in Cologne studied the logical aspects of the quantum formalism [25], while other workers (Jordan, Segal, Mackey, Varadarajan, Emch) [26,27] focused their attention on the algebraic structures, and Richard Feynman developed the path integral formulation [28].…”
Section: Magic With Neutronsmentioning
confidence: 99%
“…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. Peter Mittelstaedt and his group in Cologne studied the logical aspects of the quantum formalism [25], while other workers (Jordan, Segal, Mackey, Varadarajan, Emch) [26,27] focused their attention on the algebraic structures, and Richard Feynman developed the path integral formulation [28].…”
Section: Magic With Neutronsmentioning
confidence: 99%
“…Equation (3.8) is the typical probability rule of modern quantum mechanics in which the notion of an "effect valued measure" F ( σ) on some σ-algebra of subsets generalizes the customary concept of a projection valued measure, or equivalently of a self-adjoint operator, associated to an observable; these observables present an idealisation that is very useful to understand the basic structure of quantum mechanics, but is too strong for representing real measuring devices (Ludwig, 1983;Kraus, 1983;Holevo, 1982;Davies, 1976). A similar situation is met if one considers the statistical operator…”
Section: Physical Discussion and Conclusive Remarksmentioning
confidence: 99%
“…The standpoint according to which quantum mechanics actually is a probability theory is by now well understood, and even though it is still not in the spirit of typical textbook presentations, it has been developed and thoroughly investigated in various books and monographes (see e.g. [3][4][5][6][7][8][9][10]), to which we refer the reader for more rigorous and detailed presentations. A more concise account of similar ideas has also been given in [11].…”
Section: Quantum Mechanics As Quantum Probabilitymentioning
confidence: 99%
“…The reproducible quantity to be compared with the theory is the relative frequency according to which the preparation apparatus triggers the registration apparatus in a high enough number of repetitions of the experiment under identical circumstances. A most simple sketch of such a setup can be given by the so-called Ludwig's Kisten [3,12] preparation apparatus directed interaction −→ registration apparatus .…”
Section: Statistics Of An Experimentsmentioning
confidence: 99%