2021
DOI: 10.1007/s00601-021-01639-8
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The Investigation of Approximate Solutions of Deformed Klein–Gordon and Schrödinger Equations Under Modified More General Exponential Screened Coulomb Potential Plus Yukawa Potential in NCQM Symmetries

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Cited by 18 publications
(10 citation statements)
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“…In the search for solutions of the NR deformed Schrödinger equation DSE under the influence of several different potentials [56][57][58][59][60][61][62][63][64]. The success of this method was not limited to the DSE, but was extended to the study of various relativistic physics problems, for example, for the DKGE [65][66][67][68][69][70][71], for the DDE [72][73][74][75][76][77][78][79][80] and the deformed DKP equation [81,82]. Thus, the BS method allows us to simplify second-order linear differential equations of the DSE, DKG, DDE, and DDKPE with the Weyl-Moyal star product to the second-order linear differential SE, KGE, DE, and DKP equations with the ordinary product with simultaneous translation in the spacespace.…”
Section: Review Of Bopp's Shift Methodsmentioning
confidence: 99%
“…In the search for solutions of the NR deformed Schrödinger equation DSE under the influence of several different potentials [56][57][58][59][60][61][62][63][64]. The success of this method was not limited to the DSE, but was extended to the study of various relativistic physics problems, for example, for the DKGE [65][66][67][68][69][70][71], for the DDE [72][73][74][75][76][77][78][79][80] and the deformed DKP equation [81,82]. Thus, the BS method allows us to simplify second-order linear differential equations of the DSE, DKG, DDE, and DDKPE with the Weyl-Moyal star product to the second-order linear differential SE, KGE, DE, and DKP equations with the ordinary product with simultaneous translation in the spacespace.…”
Section: Review Of Bopp's Shift Methodsmentioning
confidence: 99%
“…Here are elements of antisymmetric ( ) real matrices, the effective Planck constant approximatively equal to reduced Planck constant , ( is the infinitesimal parameter NP, and for and ) is just an antisymmetric number while is the Kronecker symbol. The Weyl-Moyal star product of and is , which is generalized to the new deformed form by as follows, [38][39][40][41][42][43][44][45][46][47][48] which can be reduced to in the first order of NP as follows [46][47][48][49][50][51][52][53][54][55] The sum indices equal 1,2 and 3. Physically, the second term in Eq.…”
Section: Tionmentioning
confidence: 99%
“…To perform this task, the physical form of DSE, it is necessary to replace the ordinary three-dimensional Hamiltonian operators 𝐻 𝑥 , 𝑝 , the complex wave function 𝛹 𝑟 → , and energy 𝐸 with the new three Hamiltonian operators𝐻 𝑥 , 𝑝̂ , the new complex wave function𝛹 𝑟→ , and new values𝐸 , respectively. In addition to replacing the ordinary product with the Weyl-Moyal star product, which allows us to construct the DSE in the 3D-NRNCPS symmetries framework as [55][56][57][58][59][60]:…”
Section: Dse Solution For An Improved New Internal Energy Potential A...mentioning
confidence: 99%