Traditional WKB theory yields wave functions which have divergences and are not invariant under any reasonable class of transformations. This Letter presents alternative WKB wave functions which have no divergences and are symplectic invariants.
This paper shows that WKB wave function can be expressed in the form of an adiabatic expansion. To build a bridge between two widely invoked approximation schemes seems pedagogically instructive. Further, “cubic-WKB” method that has been devised in order to overcome the divergence problem of WKB can be also presented in the form of an adiabatic approximation: The adiabatic expansion of a wave function contains a certain parameter. When this parameter is adjusted so as to make the next order correction vanish approximately, the adiabatic wave function becomes equivalent to that of the “cubic-WKB”.
A method is presented for the construction of WKB wave functions that avoids explicit consideration of any matching between results pertaining to classically allowed and classically forbidden regions. The formalism is based on the maximization of a suitably defined quantal pseudoentropy, subject to the constraints posed by the expectation values of a reduced number of operators, which are evaluated according to special WKB techniques that consider expansions up to orders \ensuremath{\Elzxh} and ${\mathrm{\ensuremath{\Elzxh}}}^{2}$. The algorithm is tested with reference to the harmonic and quartic anharmonic oscillators.