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1999 J. Phys. A: Math. Gen. 32 6771-6781 doi: 10.1088/0305-4470/32/39/305
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Abstract.
Recently, a class of ![]()
-invariant quantum mechanical models described by the non-Hermitian Hamiltonian H = p2+x2(ix)
was studied. It was found that the energy levels for this theory are real for all ![]()
0. Here, the limit as ![]()
![]()
is examined. It is shown that in this limit, the theory becomes exactly solvable. A generalization of this Hamiltonian, H = p2+x2M(ix)
(M = 1,2,3, ... ) is also studied, and this ![]()
-symmetric Hamiltonian becomes exactly solvable in the large-
limit as well. In effect, what is obtained in each case is a complex analogue of the Hamiltonian for the square-well potential. Expansions about the large-
limit are obtained.
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