Abstract
In Sect. 2.11 it has been shown how a generalization of the creation and annihilation operators, known from the algebraic treatment of the harmonic oscillator (HO) problem.
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Notes
- 1.
This nomenclature is somewhat misleading, as W has the dimension of the square-root of energy, not energy like a usual potential.
- 2.
- 3.
Here \(E_0\) is the ground state energy of the conventional solution of the problems.
- 4.
This “construction of families of potentials strictly isospectral to the initial (bosonic) one” can also be interpreted as a “double Darboux general Riccati” transformation of the inverse Darboux type, going in two steps from an initial bosonic to a deformed bosonic system; for details, see [4].
- 5.
Note that the notation in [3] and the one used here differs as the quantities with and without tilde are interchanged.
- 6.
N.B.: The kinetic energy term divided by a is just identical to \(V_{\mathrm{qu}}\)!
- 7.
A similar formulation of the TISE in terms of this equation, but within a different context and with different applications, has also been given in [9]. In another paper [10, 11] the relation between the Ermakov equation (3.39) and the TISE has been extended to also include magnetic field effects and in [11] possible connections between SUSY and Ermakov theories are considered. The NL differential equation (3.39) has also been used to obtain numerical solutions of the TISE for single and double-minimum potentials as well as for complex energy resonance states; for details see [12, 13]. Here, however, we want to concentrate on the similarities between the TD and TI situation, in particular with respect to SUSY.
- 8.
For a survey of Darboux transformations , also in relation to the factorization method and SUSY quantum mechanics, see [4].
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Schuch, D. (2018). Time-Independent Schrödinger and Riccati Equations. In: Quantum Theory from a Nonlinear Perspective . Fundamental Theories of Physics, vol 191. Springer, Cham. https://doi.org/10.1007/978-3-319-65594-9_3
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