1984
DOI: 10.1016/0034-4877(84)90030-2
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Quantum mechanics in a discrete space-time

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Cited by 76 publications
(40 citation statements)
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“…We know that the number of MUBs in C d is lesser or equal to d + 1 and that the limit d + 1 is reached when d is a power of a prime [50,51,52,53,54,55,56,57,58,59]. Let us suppose that d is the power of a prime.…”
Section: Mubsmentioning
confidence: 99%
“…We know that the number of MUBs in C d is lesser or equal to d + 1 and that the limit d + 1 is reached when d is a power of a prime [50,51,52,53,54,55,56,57,58,59]. Let us suppose that d is the power of a prime.…”
Section: Mubsmentioning
confidence: 99%
“…The Wigner function W |Ψ (x, p) is a quasi-probability distribution in phase space and is normalized so that 1 2π 27) where dx dp/2π is the invariant measure in phase space (here we have takenh = 1). With these definitions we can represent a regularized version of an eigenstate of the position operatorx with mean value equal to zero, |x 0 , as a state described by the Gaussian Wigner function: 28) for which the variances of the position and momentum operators are (∆x) 2 = 1 2 e −2ξ and (∆p) 2 = 1 2 e 2ξ , respectively. The state (2.28) is a minimum uncertainty state, i.e., (∆x)(∆p) = 1 2 irrespective of the value of the squeezing parameter ξ.…”
Section: A Continuous Limitmentioning
confidence: 99%
“…Its geometric interpretation as the simplest quantum kinematic on a finite discrete configuration space formed by a periodic chain of N points was elaborated by J. Schwinger [9]. In [10] we proposed a group theoretical formulation of this quantum model as well as a finite-dimensional analogue of quantum evolution operator for a free particle.…”
Section: Quantum Mechanics In Finite-dimensional Hilbert Spacesmentioning
confidence: 99%