What are the normalizations constants of psi(x) in a finite potential box?

[j-lee00]

What are the normalizations constants of psi(x) in a finite potential box?

is there an algebraic or analytical solution.

I have the solution to the infinite box but it seems the two cases are not comparable. As in the finite box the particle does not need to be in the box?

 

[Avodyne]

There's no closed form solution. Let's set V(x)=0 for -a<x<a and V(x)=\hbar^2 \gamma^2/2m, where \gamma is a constant, for |x|>a. Then, even parity solutions are of the form \psi(x)=A\cos(kx) for |x|<a and B\exp(-\kappa|x|) for |x|>a, where k^2+\kappa^2=\gamma^2, and the energy eigenvalue is E=\hbar^2 k^2/2m. Matching \psi(x) and \psi'(x) at x=a yields the eigenvalue condition \kappa=k\tan(ka) (which must be satisfied together with k^2+\kappa^2=\gamma^2; this pair of equations can be solved graphically or numerically, but not analytically) and B/A = \exp(\kappa a)\cos(ka). You can then get the value of A by normalizing \psi(x), which will give you some expression in terms of k, \kappa, and a, with k and \kappa being fixed by the energy eigenvalue (which can only be determined graphically or numerically).

 

[j-lee00]

what is the best way to solve it computationally?