Semiclassical eigenvalues for potential functions defined on a finite interval

Abstract
It is shown that the usual WKB quantum condition for one‐dimensional potentials should be modified for problems defined on the finite interval (a,b) by adding the ’’correction’’ ΔV (x) = (h/2/8m)[π/(ba)]2/cos2 {π[x−(a+b)/2]/(ba) } to the actual potential. Numerical application shows the modified quantum condition to be a considerable improvement over the usual (i.e., unmodified) equation.
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