Abstract:Analogous to Landau quantization related to a neutral particle possessing an electric quadrupole moment, we generalize such a Landau quantization to include position-dependent mass (PDM) neutral particles. Using cylindrical coordinates, the exact solvability of PDM neutral particles with an electric quadrupole moment moving in electromagnetic fields is reported. The interaction between the electric quadrupole moment of a PDM neutral particle and a magnetic field in the absence of an electric field is analyzed … Show more
“…Moreover, we have observed that square the energies in (18) (i.e., E 2 ) resembles the Landau-type energies-squared with an irrational magnetic quantum number γ that indulges within the Aharonov-Bohm flux field effect. We may argue, therefore, that the additional compact dimension of the Kaluza-Klein theory offers quasi-Landau energy levels (e.g., [6,64,67]). Hereby, the behaviour of the energy levels E nr ,ℓ is found to follow two different trends of clustering and batching up for the curvature parameter α ≈ 0 and α ≫ 1.…”
Section: Discussionmentioning
confidence: 99%
“…It is interesting to know that this is manifestly introduced by the coupling between the compact Kaluza-Klein fifth-dimension u and the ϕ coordinate. As such, we may argue that the additional compact dimension of the Kaluza-Klein theory offers quasi-Landau energy levels (e.g., [6,64,67]). Moreover, one should be aware that the four possible KG-oscillators' settings discussed above, with some straightforward parametric substitutions, admit exact solvability as in (18) and (19).…”
Section: Kg-oscillator In Cosmic String Spacetime Within Kkt: Recycle...mentioning
In the cosmic string spacetime and within Kaluza-Klein theory (KKT) backgrounds (indulging magnetic and Aharonov-Bohm flux fields), we introduce and study position-dependent mass (PDM) Klein-Gordon (KG) oscillators. The effective PDM is introduced as a deformation/defect in the momentum operator. We show that there are four different ways to obtain KGoscillator. Two of which are readily known and the other two are obtained as byproducts of PDM settings. Next, we provide a thorough analysis on the corresponding spectra under different parametric effects, including the curvature parameter's effect. Such analysis is used as a reference/lead model which is used in the discussion of different PDM KG-oscillators models: a mixed powerlaw and exponential type PDM model that yields a pseudo-confined PDM KG-oscillator in cosmic string spacetime within KKT (i.e., the PDM KG-oscillators are confined in their own PDM manifested Cornell-type confinement), and a PDM KG-oscillator confined in a Cornell-type potential.Moreover, we extend our study and discuss a non-Hermitian PT -symmetric PDM-Coulombic-type KG-particle model in cosmic string spacetime within KKT.
“…Moreover, we have observed that square the energies in (18) (i.e., E 2 ) resembles the Landau-type energies-squared with an irrational magnetic quantum number γ that indulges within the Aharonov-Bohm flux field effect. We may argue, therefore, that the additional compact dimension of the Kaluza-Klein theory offers quasi-Landau energy levels (e.g., [6,64,67]). Hereby, the behaviour of the energy levels E nr ,ℓ is found to follow two different trends of clustering and batching up for the curvature parameter α ≈ 0 and α ≫ 1.…”
Section: Discussionmentioning
confidence: 99%
“…It is interesting to know that this is manifestly introduced by the coupling between the compact Kaluza-Klein fifth-dimension u and the ϕ coordinate. As such, we may argue that the additional compact dimension of the Kaluza-Klein theory offers quasi-Landau energy levels (e.g., [6,64,67]). Moreover, one should be aware that the four possible KG-oscillators' settings discussed above, with some straightforward parametric substitutions, admit exact solvability as in (18) and (19).…”
Section: Kg-oscillator In Cosmic String Spacetime Within Kkt: Recycle...mentioning
In the cosmic string spacetime and within Kaluza-Klein theory (KKT) backgrounds (indulging magnetic and Aharonov-Bohm flux fields), we introduce and study position-dependent mass (PDM) Klein-Gordon (KG) oscillators. The effective PDM is introduced as a deformation/defect in the momentum operator. We show that there are four different ways to obtain KGoscillator. Two of which are readily known and the other two are obtained as byproducts of PDM settings. Next, we provide a thorough analysis on the corresponding spectra under different parametric effects, including the curvature parameter's effect. Such analysis is used as a reference/lead model which is used in the discussion of different PDM KG-oscillators models: a mixed powerlaw and exponential type PDM model that yields a pseudo-confined PDM KG-oscillator in cosmic string spacetime within KKT (i.e., the PDM KG-oscillators are confined in their own PDM manifested Cornell-type confinement), and a PDM KG-oscillator confined in a Cornell-type potential.Moreover, we extend our study and discuss a non-Hermitian PT -symmetric PDM-Coulombic-type KG-particle model in cosmic string spacetime within KKT.
“…This would consequently enrich the class of exactly solvable dynamical systems within the standard Lagrangian/Hamiltonian settings. Moreover, one should be aware that when equation ( 35) is multiplied by qi and summed over i = 1, 2, • • • , n, it would yield (43) or equivalently (45).…”
Section: B N-dimensional Pdm ḣ-Invariancementioning
confidence: 99%
“…Which is, in fact, a very interesting equation for both physics and mathematics [1][2][3][4][5][6][7][8][9][10][11]. The linearizability and isochronicity of which have invited a vast number of interesting research studies in many fields (c.f., e.g., [35][36][37][38][39][40][41][42][43][44][45]). Tiwari et al [2] and Lakshmanan and Chandrasekar [3], for example, have used Lie point symmetries and asserted that in the case of eight parameter symmetry group, the one-dimensional quadratic Liénard type equation ( 3) is linearizable and isochronic.…”
Within the standard Lagrangian settings (i.e., the difference between kinetic and potential energies), we discuss and report isochronicity, linearizability and exact solvability of some n-dimensional nonlinear position-dependent mass (PDM) oscillators. In the process, negative the gradient of the PDM-potential force field is shown to be no longer related to the time derivative of the canonical momentum, p = m (r) ṙ, but it is rather related to the time derivative of the pseudo-momentum, π (r) = m (r)ṙ (i.e., Noether momentum). Moreover, using some point transformation recipe, we show that the linearizability of the n-dimensional nonlinear PDM-oscillators is only possible for n = 1 but not for n ≥ 2. The Euler-Lagrange invariance falls short/incomplete for n ≥ 2 under PDM settings. An alternative invariance is therefore sought in the so called, hereinafter, n-dimensional PDM Ḣ-invariance (i.e., time derivative of the Hamiltonian). Such invariance, in addition to Newtonian invariance of Mustafa [42] authorizes, in effect, the use of the exact solutions of one system to find the solutions of the other. A sample of isochronous n-dimensional nonlinear PDM-oscillators examples are reported.
“…In addition, it is also shown the coherent states for the harmonic oscillator satisfy the minimization of the Heisenberg's uncertainty principle. 16 Complementary, another important issue in quantum mechanics is the concept of position-dependent mass (PDM), which has attracted the attention along the decades due its wide applicability in: semiconductor heterostructures, [17][18][19][20][21][22][23][24] nonlinear optics, 25 quantum liquids, 26 many-body theory, 27 molecular physics, 28 Wigner functions, 29 quantum information, 30 relativistic quantum mechanics, 31 Dirac equation, 32 superintegrable systems, 33 nuclear physics, 34 magnetic monopoles, 35 Landau quantization, 36 factorization and supersymmetry methods, [37][38][39][40][41] coherent states, [42][43][44][45] etc.…”
We study the classical and quantum oscillator in the context of a non-additive (deformed) displacement operator, associated with a position-dependent effective mass, by means of the supersymmetric formalism. From the supersymmetric partner Hamiltonians and the shape invariance technique we obtain the eigenstates and the eigenvalues along with the ladders operators, thus showing a preservation of the supersymmetric structure in terms of the deformed counterpartners. The deformed space in supersymmetry allows to characterize position-dependent effective mass, uniform field interactions and to obtain a generalized uncertainty relation (GUP) that behaves as a distinguishability measure for the coherent states, these latter satisfying a periodic evolution of the GUP corrections.
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