1996
DOI: 10.1016/s1355-2198(96)00002-0
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Modal interpretations, decoherence and measurements

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Cited by 57 publications
(34 citation statements)
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“…In other words, after the decoherence time the off-diagonal elements of ρ ( ) M t are small independently of the original disturbance (for a full argument, see Bacciagaluppi and Hemmo 1996; for difficulties in continuous models, see Bacciagaluppi 2000).…”
Section: Modal Interpretations and Decoherencementioning
confidence: 99%
“…In other words, after the decoherence time the off-diagonal elements of ρ ( ) M t are small independently of the original disturbance (for a full argument, see Bacciagaluppi and Hemmo 1996; for difficulties in continuous models, see Bacciagaluppi 2000).…”
Section: Modal Interpretations and Decoherencementioning
confidence: 99%
“…For this reason Kiefer and Polarski claim "Then the quantum system is effectively equivalent to the classical random system, which is an ensemble of classical trajectories with a certain probability associated to each of them" ( [71] pp. 4) A concrete example in which f k2 and g k1 tend to zero, is the perturbation on de Sitter space [72]. When the decaying mode becomes vanishingly small; when this mode is neglected we are in the limit of a random stochastic process.…”
Section: Decoherence Without Decoherencementioning
confidence: 99%
“…It has been fruitfully applied in many areas of physics and supplies the basis of new technological developments. In the foundations of physics community, EID has been viewed as a relevant element for the interpretation of quantum mechanics ( [3], [4]) and for the explanation of the emergence of classicality from the quantum world ( [5], [6], [7], [8]). …”
Section: Introductionmentioning
confidence: 99%
“…And, unlike orthodox quantum theory, no miraculous collapse is needed to solve the measurement problem. Instead, after a typical unitary 'measurement' interaction between two parts of the universe -O the 'measured' system, and A the apparatus -decoherence induced by A's coupling to the environment O ∪ A will force the density operator D A of the apparatus to diagonalize in a basis extremely close to one which diagonalizes the pointer observable of A [14]. Thus, after the measurement, the definite-valued observables in M A will be such that the pointer points!…”
Section: The Modal Interpretation Of Nonrelativistic Quantum Theorymentioning
confidence: 99%