2007
DOI: 10.1088/1751-8113/40/12/s14
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Quantum theory: the role of microsystems and macrosystems

Abstract: We stress the notion of statistical experiment, which is mandatory for quantum mechanics, and recall Ludwig's foundation of quantum mechanics, which provides the most general framework to deal with statistical experiments giving evidence for particles. In this approach particles appear as interaction carriers between preparation and registration apparatuses. We further briefly point out the more modern and versatile formalism of quantum theory, stressing the relevance of probabilistic concepts in its formulati… Show more

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Cited by 6 publications
(6 citation statements)
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References 46 publications
(56 reference statements)
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“…In particular the analysis of the interaction of a quantum system with a structured reservoir, performed via a time-convolutionless projection operator technique relying on the use of correlated projection operators adapted to the structured reservoir [7], has led to point out a generalized Lindblad structure [8]. This generalized Lindblad structure describes a non-Markovian dynamics on states which are given by classical convex mixtures of subcollections, that is positive trace class operators with trace equal or less than one, naturally appearing in the description of quantum experiments [9]. Master equations of this form have already been proposed in an utterly different context in order to introduce the notion of event in the description of quantum mechanical systems [10], for the purpose of better understanding the interplay between classical and quantum description of physical reality.…”
Section: Introductionmentioning
confidence: 99%
“…In particular the analysis of the interaction of a quantum system with a structured reservoir, performed via a time-convolutionless projection operator technique relying on the use of correlated projection operators adapted to the structured reservoir [7], has led to point out a generalized Lindblad structure [8]. This generalized Lindblad structure describes a non-Markovian dynamics on states which are given by classical convex mixtures of subcollections, that is positive trace class operators with trace equal or less than one, naturally appearing in the description of quantum experiments [9]. Master equations of this form have already been proposed in an utterly different context in order to introduce the notion of event in the description of quantum mechanical systems [10], for the purpose of better understanding the interplay between classical and quantum description of physical reality.…”
Section: Introductionmentioning
confidence: 99%
“…[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: 91%
“…[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: 91%
“…Such a condition typically applies when a symmetry, available in the system one is studying, is not spoiled by the transformations brought about on the system by letting it interact with another system, be it a reservoir or a measuring apparatus. The possibility of giving a general solution of the covariance equation (11) obviously depends on the unitary representation of the group and on the class of mappings considered, possibly giving very detailed information on the general structure of such mappings.…”
Section: Covariancementioning
confidence: 99%