Abstract

In this article, we write the general form of the quasiexactly solvable Hamiltonian of g 2 algebra via one special representation in the x–y two-dimensional space. Then, by choosing an appropriate set of coefficients and making a gauge rotation, we show that this Hamiltonian leads to the solvable Poschl–Teller model on an open infinite strip. Finally, we assign g 2 hidden algebra to the Poschl–Teller potential and obtain its spectrum by using the representation space of g 2 algebra.

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