2018
DOI: 10.1063/1.4986964
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Noncommutative mapping from the symplectic formalism

Abstract: The Bopp's shifts will be generalized through symplectic formalism. A special procedure, like a "diagonalization", which drives the completely deformed symplectic matrix to the standard symplectic form was found as suggested by Faddeev-Jackiw.Consequently, the correspondent transformation matrix guides the mapping from commutative to noncommutative (NC) phase-space coordinates. The Bopp's shifts may be directly generalized from this mapping. In this context, all the NC and scale parameters, introduced into the… Show more

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Cited by 21 publications
(13 citation statements)
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“…Quantum gravity, string theory, and the divergence problem of the standard model new data made this new quantum theory a refuge for physicists to find solutions and discoveries hoped for on the other hand [38][39][40][41][42][43][44][45][46][47][48]. In recent years, a lot attention has been drawn to this development [49][50][51][52][53][54][55][56][57][58][59].…”
Section: Introductionmentioning
confidence: 99%
“…Quantum gravity, string theory, and the divergence problem of the standard model new data made this new quantum theory a refuge for physicists to find solutions and discoveries hoped for on the other hand [38][39][40][41][42][43][44][45][46][47][48]. In recent years, a lot attention has been drawn to this development [49][50][51][52][53][54][55][56][57][58][59].…”
Section: Introductionmentioning
confidence: 99%
“…is the noncommutative parameter) which is an infinitesimal parameter if compared to the energy values and elements of antisymmetric real matrices and μ ν is the identity matrix. The symbol denotes the Weyl Moyal star product, which is generalized between two ordinary functions to the new deformed form which expressed with the Weyl Moyal star product in the symmetries of NCQM as follows [37][38][39][40][41][42][43] :…”
Section: Introductionmentioning
confidence: 99%
“…The coupling L Θ equals L x Θ 12 + L y Θ 23 + L z Θ 13 , where L x , L y , and L z are the usual components of angular momentum operator L in RQM while the new noncommutativity parameter Θ µν equals θ µν /2. The new structure of (RNCQM) based on new covariant noncommutative canonical commutations relations (CNCCRs) in Schrödinger, Heisenberg and interactions pictures (SP, HP, and IP), respectively, as follows [36][37][38][39][40][41][42][43][44][45][46]:…”
Section: Introductionmentioning
confidence: 99%