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2015
DOI: 10.5506/aphyspolb.46.1309
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Remarks on Mathematical Foundations of Quantum Mechanics

Abstract: We show that the set-theoretic forcing is the essential part of the continuous measurement of a suitably rich Boolean algebra of quantum observables. The Boolean algebra structure of quantum observables enables us to give a classical and geometric meaning to the results of measurements of the observables. The measurement takes place in the semiclassical state of the system which is the generic filter added by a forcing to the ZFC model based on the Borel measure algebra. The analogue of the semiclassical state… Show more

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Cited by 5 publications
(8 citation statements)
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“…Without any cutoff imposed, this integral is UV-divergent. However, in our model, it holds that [8,9] Theorem 2. Zero-energy modes of quantum fields have vanishing contributions to the gravitational vacuum energy.…”
Section: The Physics Of Forcingmentioning
confidence: 87%
See 2 more Smart Citations
“…Without any cutoff imposed, this integral is UV-divergent. However, in our model, it holds that [8,9] Theorem 2. Zero-energy modes of quantum fields have vanishing contributions to the gravitational vacuum energy.…”
Section: The Physics Of Forcingmentioning
confidence: 87%
“…Moreover, forcing can be regarded as a technique for exploring the structure of the real line rather than proving independence results in formal set theory. Set-theoretic forcing as a tool in QM has already been identified and used by several authors, such as P. Benioff [4], G. Takeuti [5], M. Ozawa [6,7], W. Boos [2], R. Van Wesep [1], and the present authors [8][9][10][11][12].…”
Section: Classical Large-scale Coordinates From Quantum Regimementioning
confidence: 99%
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“…This section is the summary of our previous article regarding the forcing emerging from QM. An interested reader is referred to [6] for a more detailed treatment. A forcing can be seen as the deriving property of some Boolean algebra 1 .…”
Section: Forcing In Qmmentioning
confidence: 99%
“…A forcing can be seen as the deriving property of some Boolean algebra 1 . By B, we denote some Boolean algebra of projections chosen from the lattice of projections L(H) on a Hilbert space H. The spectral theorem, in general, gives the correspondence between the algebra of self-adjoint (s-a) operators which are in the Boolean algebra B [6,7] and the measure algebra defined on the Borel subsets of X = R 3 . Actually, there exists the isomorphism between the algebra B generating the family of s-a operators {A α } and the measure algebra of the space 2 (X, µ).…”
Section: Forcing In Qmmentioning
confidence: 99%