dingo_d
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Homework Statement
I have solved the problem of an infinite square well with a delta potential in the middle, what I got in the end is:
[tex]\cot(\frac{\sqrt{2 m E}}{\hbar}a)=-\frac{\Omega\hbar a \sqrt{2m E}}{2mE a}[/tex]
, where a is the width of the well, m the mass of the particle in it, E the energy eigenvalue, and [tex]\Omega[/tex] some parameter that was with the delta potential.
Now I need to solve that equation and I have no idea how to do that :\
I'm not much of a numerical solver :\
Anywho the solution to Schrödinger eq. is:
[tex]u_n^+(x) =<br /> \begin{cases}<br /> A\sin(k_n^+(x+a)) & \text{if } -a\leq x < 0 \\<br /> -A\sin(k_n^+(x-a)) & \text{if } 0< x \leq a<br /> \end{cases}[/tex]
And the [tex]k_n^+=\frac{n\pi}{2a}[/tex], where [tex]n=\pm 2,\pm 4,\ldots[/tex]