Symmetrized exponential oscillator
arXiv:1609.00166 · doi:10.1142/S0217732316501959
Abstract
Several properties of bound states in potential are studied. Firstly, with the emphasis on the reliability of our arbitrary-precision construction, wave functions are considered in the two alternative (viz., asymptotically decreasing or regular) exact Bessel-function forms which obey the asymptotic or matching conditions, respectively. The merits of the resulting complementary transcendental secular equation approaches are compared and their applicability is discussed.
14 pp., 6 figures
References in corpus (15)
- Supersymmetry and Quantum Mechanics
- Schrödinger operators with complex potential but real spectrum
- PT symmetric square well
- One-Dimensional Quasi-Exactly Solvable Schrödinger Equations
- Exact solution of the Schrödinger equation for the inverse square root potential
- MHD alpha^2-dynamo, Squire equation and PT-symmetric interpolation between square well and harmonic oscillator
- Spontaneous breakdown of PT symmetry in the solvable square-well model
- Coupled-channel version of PT-symmetric square well
- One-dimensional Schrödinger equation with non-analytic potential and its exact Bessel-function solvability
- Morse potential, symmetric Morse potential and bracketed bound-state energies
- Symmetrized quartic polynomial oscillators and their partial exact solvability
- Quantum star-graph analogues of PT-symmetric square wells
- PT-supersymmetric partner of a short-range square well
- Accurate calculation of the complex eigenvalues of the Schrödinger equation with an exponential potential
- Markov constant and quantum instabilities
Cited by in corpus (6)
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- Exactly solvable piecewise analytic double well potential and its dual single well potential
- Displaced harmonic oscillator as a benchmark double-well quantum model
- Swanson Hamiltonian: non-PT-symmetry phase
- The third five-parametric hypergeometric quantum-mechanical potential