2001
DOI: 10.1088/0305-4470/34/32/313
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Supersymmetric approach for generating quasi-exactly solvable potentials with arbitrary two known eigenstates

Abstract: Using supersymmetric quantum mechanics we construct the quasiexactly solvable (QES) potentials with arbitrary two known eigenstates. The QES potential and the wave functions of the two energy levels are expressed by some generating function the properties of which determine the state numbers of these levels. Choosing different generating functions we present a few explicit examples of the QES potentials.

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Cited by 5 publications
(5 citation statements)
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“…On starting from some assumption for the latter, it is possible to construct QES potentials with two known eigenstates (the ground and first excited states again). This method has also been generalized for generating QES potentials with arbitrary two known eigenstates [32], as well as QES potentials with three known eigenstates [33].…”
Section: Introductionmentioning
confidence: 99%
“…On starting from some assumption for the latter, it is possible to construct QES potentials with two known eigenstates (the ground and first excited states again). This method has also been generalized for generating QES potentials with arbitrary two known eigenstates [32], as well as QES potentials with three known eigenstates [33].…”
Section: Introductionmentioning
confidence: 99%
“…In this paper we develop a simple method for generation of QES potentials with two known eigenstates in arbitrary dimension. For one-dimensional case the problem of constructing QES potential with two known levels was solved completely in the frame of SUSY quantum mechanics [33,34,35] or using a simple method in which two wave functions are chosen in such a way that they lead to the same potential [36,37]. Just this method will be generalized for multidimensional case.…”
Section: Introductionmentioning
confidence: 99%
“…Note that in fact the idea of the papers [33,34,35,36,37] is based on the inverse method. For the first time this method was used by Ushveridze [14] for construction QES potentials.…”
Section: Introductionmentioning
confidence: 99%
“…A distinctive feature of this method is that in contrast with other ones, it does not require the knowledge of an initial QES potential for constructing a new one. Later on, the procedure was extended to deal with QES potentials with two arbitrary eigenstates [14] or with three eigenstates [15].…”
Section: Introductionmentioning
confidence: 99%