
doi: 10.1007/bf02724031
The Schrodinger equation with a new nonstationary potential of the type 1/2ω2(t)r2 +f(θ, ϕ)r−2 is solved exactly. Normalized solutions and transition amplitudes between energy eigenstates are expressed in terms of Jacobi and Laguerre polynomials. Integrals of the motion are considered.
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