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dingo_d
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Homework Statement
I am given the modified Poschl-Teller potential:
[tex]V(x)=-\frac{U_0}{\cosh^2(\alpha x)}[/tex]. I have to make WKB approximation of bound energy states and compare it to exact solution (analytical and numerical).
Homework Equations
Exact solution is given:
[tex]E_n=-\frac{\alpha^2\hbar^2}{2m}\left[\frac{1}{2}\sqrt{\frac{8m U_0}{\alpha^2\hbar^2}+1}-\left(n+\frac{1}{2}\right)\right]^2,\quad n\in\mathbb{Z^+}[/tex]
WKB energy approximation is calculated from integral:
[tex]\int\limits_{x_1}^{x_2}\sqrt{2m(E-V(x))}dx=\left(n+\frac{1}{2}\right)\hbar\pi[/tex]
[tex]x_1,\ x_2[/tex] are the turning points, places where [tex]V(x)=E[/tex].
The Attempt at a Solution
I found the solution in one article in Annals of Physics and it's:
[tex]E_n=-\frac{\alpha^2\hbar^2}{2m}\left[\sqrt{\frac{2m U_0}{\alpha^2\hbar^2}}-\left(n+\frac{1}{2}\right)\right]^2,\quad n\in\mathbb{Z^+}[/tex]
And when I do the numerics via Python and Mathematica I get nice results (with Planck cons=m=alpha=1, and U_0=8) for ground state (n=0):
[tex]E_0^{exact/num}=-6.2344,\quad E_0^{WKB}=-6.125[/tex]. So that really is the result. But how do I solve that nasty integral?!
It's:
[tex]\int\limits_{x_1}^{x_2}\sqrt{2m\left(E+\frac{U_0}{\cosh^2(\alpha x)}\right)}dx[/tex]
Plus the turning points are something like arccosh which is a multivalued function.
Do I solve this by complex integration? And if so, how? Because usually the limits of complex integrals are usually something like infinities...
I tried substitution, [tex]z=\cosh^2(\aplha x)[/tex] but I had no luck. Plus the limits of the integral ends up the same when I substitute (probably because of the multivaluedness) :\
Any ideas?