Abstract:The classical and quantum mechanical correspondence for constant mass settings is used, along with some point canonical transformation, to find the position-dependent mass (PDM) classical and quantum Hamiltonians. The comparison between the resulting quantum PDM-Hamiltonian and the von Roos PDM-Hamiltonian implied that the ordering ambiguity parameters of von Roos are strictly determined. Eliminating, in effect, the ordering ambiguity associated with the von Roos PDM-Hamiltonian. This, consequently, played a v… Show more
“…wherep = −i∂ x is the regular textbook constant mass momentum operator used in (69) and (70). Finally, the PDM quantum supersymmetric approach with the asymptotic geometrical classical oscillator correspondence by Cruz et al [21], the factorization approach by Mustafa and Mazharimousavi [27], the construction of the PDM-momentum operator approach by Mustafa and Algadhi [10], and the current PDM creation and annihilation oscillator operators approach, all confirm and emphasize that the PDM-Hamiltonian H 1 of (29) is the only surviving one out of the von Roos PDM Hamiltonians. However, the quantization approach of the PDM Noether momentum by Cariñena et al [34], and our analysis and discussions in the current methodical proposal suggest thatĤ 2 of (68) is not only correlated withĤ 1 but also more simplistic user-friendly thanĤ 1 that of (63).…”
The exact solvability and impressive pedagogical implementation of the harmonic oscillator's creation and annihilation operators make it a problem of great physical relevance and the most fundamental one in quantum mechanics. So would be the position-dependent mass (PDM) oscillator for the PDM quantum mechanics. We, hereby, construct the PDM creation and annihilation operators for the PDM oscillator via two different approaches. First, via von Roos PDM Hamiltonian and show that the commutation relation between the PDM creation + and annihilation operators, [Â, + ] = 1 ⇔ + − 1/2 = + + 1/2, not only offers a unique PDM-Hamiltonian H1 but also suggests a PDM-deformation in the coordinate system. Next, we use a PDM point canonical transformation of the textbook constant mass harmonic oscillator analog and obtain yet another set of PDM creationB + and annihilationB operators, hence an "apparently new" PDM-HamiltonianĤ2 is obtained. The "new" PDM-HamiltonianĤ2 turned out to be not only correlated withĤ1 but also represents an alternative and most simplistic user-friendly PDM-Hamiltonian, H = p/ 2m (x) 2 + V (x) ;p = −i ∂x, that has never been reported before.
“…wherep = −i∂ x is the regular textbook constant mass momentum operator used in (69) and (70). Finally, the PDM quantum supersymmetric approach with the asymptotic geometrical classical oscillator correspondence by Cruz et al [21], the factorization approach by Mustafa and Mazharimousavi [27], the construction of the PDM-momentum operator approach by Mustafa and Algadhi [10], and the current PDM creation and annihilation oscillator operators approach, all confirm and emphasize that the PDM-Hamiltonian H 1 of (29) is the only surviving one out of the von Roos PDM Hamiltonians. However, the quantization approach of the PDM Noether momentum by Cariñena et al [34], and our analysis and discussions in the current methodical proposal suggest thatĤ 2 of (68) is not only correlated withĤ 1 but also more simplistic user-friendly thanĤ 1 that of (63).…”
The exact solvability and impressive pedagogical implementation of the harmonic oscillator's creation and annihilation operators make it a problem of great physical relevance and the most fundamental one in quantum mechanics. So would be the position-dependent mass (PDM) oscillator for the PDM quantum mechanics. We, hereby, construct the PDM creation and annihilation operators for the PDM oscillator via two different approaches. First, via von Roos PDM Hamiltonian and show that the commutation relation between the PDM creation + and annihilation operators, [Â, + ] = 1 ⇔ + − 1/2 = + + 1/2, not only offers a unique PDM-Hamiltonian H1 but also suggests a PDM-deformation in the coordinate system. Next, we use a PDM point canonical transformation of the textbook constant mass harmonic oscillator analog and obtain yet another set of PDM creationB + and annihilationB operators, hence an "apparently new" PDM-HamiltonianĤ2 is obtained. The "new" PDM-HamiltonianĤ2 turned out to be not only correlated withĤ1 but also represents an alternative and most simplistic user-friendly PDM-Hamiltonian, H = p/ 2m (x) 2 + V (x) ;p = −i ∂x, that has never been reported before.
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 for two different radial cylindrical PDM settings. Next, two particular cases of radial electric fields ( − → E = λ ρ ρ and − → E = λρ 2 ρ) are considered to investigate their influence on the Landau quantization (of this system using the same models of PDM settings). The exact eigenvalues and eigenfunctions for each case are analytically obtained.
“…where − → A ( − → r ) is the vector potential, eϕ ( − → r ) is a scalar potential and V ( − → r ) is any other potential energy than the electricomagnetic one. In a subsequent work, moreover, Mustafa and Algadhi [11] have constructed and defined the PDM-momentum operator as…”
Using azimuthally symmetrized cylindrical coordinates, we consider some positiondependent mass (PDM) charged particles moving in position-dependent (PD) magnetic and Aharonov-Bohm flux fields. We focus our attention on PDM-charged particles with m ( − → r ) = g (ρ) = η f (ρ) exp (−δρ) (i.e., the PDM is only radially dependent) moving in an inverse power-law-type radial PD-magnetic fieldsUnder such settings, we consider two almost-quasi-free PDM-charged particles (i.e., no interaction potential, V ( − → r ) = 0) endowed with g (ρ) = η/ρ and g (ρ) = η/ρ 2 . Both yield exactly solvable Schrödinger equations of Coulombic nature but with different spectroscopic structures. Moreover, we consider a Yukawa-type PDM-charged particle with g (ρ) = η exp (−δρ) /ρ moving not only in the vicinity of the PD-magnetic and Aharonov-Bohm flux fields but also in the vicinity of a Yukawa plus a Kratzer type potential force field V (ρ) = −V• exp (−δρ) /ρ−V 1 /ρ+V 2 /ρ 2 . For this particular case, we use the Nikiforov-Uvarov (NU) method to come out with exact analytical eigenvalues and eigenfunctions. Which, in turn, recover those of the almost-quasi-free PDM-charged particle with g (ρ) = η/ρ for V• = V 1 = V 2 = 0 = δ.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.