2014
DOI: 10.1063/1.4884299
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Generalized space and linear momentum operators in quantum mechanics

Abstract: We propose a modification of a recently introduced generalized translation operator, by including a q-exponential factor, which implies in the definition of a Hermitian deformed linear momentum operatorpq, and its canonically conjugate deformed position operatorxq. A canonical transformation leads the Hamiltonian of a position-dependent mass particle to another Hamiltonian of a particle with constant mass in a conservative force field of a deformed phase space. The equation of motion for the classical phase sp… Show more

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Cited by 42 publications
(41 citation statements)
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References 26 publications
(29 reference statements)
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“…We consider that the techniques employed in this work could stimulate the seek of other generalizations of classical and quantum mechanical aspects, as has been reported in recent research studies by means of the q-algebra. 7,[48][49][50][51][52][53][54][55][56]…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…We consider that the techniques employed in this work could stimulate the seek of other generalizations of classical and quantum mechanical aspects, as has been reported in recent research studies by means of the q-algebra. 7,[48][49][50][51][52][53][54][55][56]…”
Section: Discussionmentioning
confidence: 99%
“…Complementarily, it has been found that the mathematical foundations of the PDM systems rely on the assumption of the noncommutativity between the mass operator m(x) and the linear momentum operatorp, thus giving place to the ordering problem for the kinetic energy operator. 4,[40][41][42][43][44][45][46][47] In addition, the development of generalized translation operators motivated the introduction of a positiondependent linear momentum for characterizing a particle with a PDM 7,[48][49][50][51][52][53][54][55][56] that can be related to a generalized algebraic structure (called q-algebra 57 ) inherited from the mathematical background of nonextensive statistics. 58 Concerning these formal structures, the κ-deformed statistics, originated from the κ-exponential and κ-logarithm functions, allows us to develop an algebraic structure, called κ-algebra, [59][60][61][62][63][64][65][66][67][68][69][70][71][72][73][74] with similar properties to those of the q-algebra.…”
Section: Introductionmentioning
confidence: 99%
“…= e z ) (and its associated q-Gaussian [78]) has already emerged in a considerable amount of nonextensive and similar systems (see [6,38,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104] among others), as the appropriate generalization of the exponential one (and its associated Gaussian) (with regard to the nonlinear quantum equations introduced in [103], see also [105,106,107,108,109,110,111,112,113,114,115]). Therefore, it appears as rather natural to conjecture that, in some sense that remains to be precisely defined, the LDT expression e −r 1 N becomes generalized into something close to e −rqN q (q ∈ R), where the generalized rate function r q should be some generalized entropic quantity per particle.…”
Section: Towards a Generalized Large-deviation Theorymentioning
confidence: 99%
“…Electric mass ' ' and magnetic mass 2 can be thought of as two quantum states. The quantum operator [9,10] for mass can be written as…”
Section: Initial Concepts Of the New Theorymentioning
confidence: 99%