2013
DOI: 10.1063/1.4835615
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Laplace-Runge-Lenz vector in quantum mechanics in noncommutative space

Abstract: The main point of this paper is to examine a "hidden" dynamical symmetry connected with the conservation of Laplace-Runge-Lenz vector (LRL) in the hydrogen atom problem solved by means of noncommutative quantum mechanics (NCQM). The basic features of NCQM will be introduced to the reader, the key one being the fact that the notion of a point, or a zero distance in the considered configuration space, is abandoned and replaced with a "fuzzy" structure in such a way that the rotational invariance is preserved.The… Show more

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Cited by 35 publications
(45 citation statements)
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“…The vectorŴ i has not been introduced yet, but it turns out to be closely related to the kinetic part of the Laplace-Runge-Lenz vector, see Ref. 13. Time derivative of velocity expectation is fully determined by expectation of this commutator (Ehrenfest theorem).…”
Section: The Acceleration Operatormentioning
confidence: 99%
“…The vectorŴ i has not been introduced yet, but it turns out to be closely related to the kinetic part of the Laplace-Runge-Lenz vector, see Ref. 13. Time derivative of velocity expectation is fully determined by expectation of this commutator (Ehrenfest theorem).…”
Section: The Acceleration Operatormentioning
confidence: 99%
“…In next section, it will allow us to define the kinetic part of a scalar field theory action as in the commutative case, in terms of the ordinary Laplacian. The closure condition (5.7), written as 5) implies that the integrand is a total derivative, i.e., there exist such a bidifferential operator…”
Section: Jhep08(2015)024mentioning
confidence: 99%
“…Besides their appearence in the quantum gravity context, noncommutative structures on R 3 are very interesting because of their application in the quantization of standard dynamical systems as for example the hydrogen atom [4][5][6]. As for their implications in quantum field theory, such as their renormalization properties and the UV/IR behaviour, which are quite different from noncommutative field theories on Moyal space-time, they are analyzed in [7][8][9]within the noncommutative space R 3 λ first introduced in [10].…”
Section: Introductionmentioning
confidence: 99%
“…Depending on the construction that is used, it can be totally [24] or partially [9] broken, or even totally retained [25].…”
Section: The Relation L · M = 0 and The Energy Shellmentioning
confidence: 99%