2016
DOI: 10.1007/s11229-016-1175-0
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Quantum mechanics over sets: a pedagogical model with non-commutative finite probability theory as its quantum probability calculus

Abstract: This paper shows how the classical finite probability theory (with equiprobable outcomes) can be reinterpreted and recast as the quantum probability calculus of a pedagogical or toy model of quantum mechanics over sets (QM/sets). There have been several previous attempts to develop a quantum-like model with the base field of C replaced by Z2. Since there are no inner products on vector spaces over finite fields, the problem is to define the Dirac brackets and the probability calculus. The previous attempts all… Show more

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Cited by 15 publications
(17 citation statements)
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“…A concrete example of the #1 and #2 ways to go from equivalence to identity is the derivation of the Maxwell-Boltzmann distribution and the Bose-Einstein distribution as in Feller [8, pp. 20-1] or Ellerman [5]. This treatment is illuminated by the classical and quantum version of a symmetry operation.…”
Section: The Connection To Interpreting Symmetry Operationsmentioning
confidence: 99%
See 1 more Smart Citation
“…A concrete example of the #1 and #2 ways to go from equivalence to identity is the derivation of the Maxwell-Boltzmann distribution and the Bose-Einstein distribution as in Feller [8, pp. 20-1] or Ellerman [5]. This treatment is illuminated by the classical and quantum version of a symmetry operation.…”
Section: The Connection To Interpreting Symmetry Operationsmentioning
confidence: 99%
“…Let f : U ! R be a real-valued random variable with distinct values i for i = 1; :::; m and let = fB i g i=1;:::;m where B i = f 1 ( i ), be the partition of U according to the f -values as in [5]. As before with incidence matrices, we want the classi…cation or di¤erentiation of (S) according to the di¤erent f -values.…”
Section: From Incidence To Density Matricesmentioning
confidence: 99%
“…The above machinery from the classical cases formulated over Z n 2 gives a pedagogical (or "toy") model of QM-"quantum mechanics over sets." [15]…”
Section: The Quantum Casementioning
confidence: 99%
“…Given two DSDs = fV i g i2I and = fW j g j2J , their proto-join is the set of non-zero subspaces fV i \ W j jV i \ W j 6 = f0gg (i;j)2I J (which do not necessarily form a DSD). If the two DSDs and were de…ned as the eigenspace DSDs of two diagonalizable operators, then the space spanned by the proto-join would be the space spanned by the simultaneous eigenvectors of the two operators, and that space is the kernel of the commutator of the two operators [6]. If the two operators commuted, then their commutator is the zero operator whose kernel is the whole space so the proto-join would span the whole space.…”
Section: Compatibility Of Dsdsmentioning
confidence: 99%
“…For instance, in the pedagogical model of "quantum mechanics over sets" or QM/Sets [6], the vector space is Z n 2 so the only diagonalizable operators are projection operatorsP : Z n 2 ! Z n 2 .…”
Section: Introductionmentioning
confidence: 99%