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We discussed the discussion problem from yesterday (Oct 6). We have the potential:
<math>V(x)= -\alpha[\delta(x-a)+\delta(x+a)] </math>
We can separate <math>\psi(x)</math> into three regions:
<math>\psi_1(x)</math>, where x < -a
<math>\psi_2(x)</math>, where -a < x < a
<math>\psi_3(x)</math>, where x > a
The wave functions end up being:
<math>\psi_1(x)=Ae^{(kx)}</math>
<math>\psi_2(x)=Be^{(kx)}+Ce^{(-kx)}</math>
<math>\psi_3(x)=De^{(-kx)}</math>
with <math>k^2=-\frac{2mE}{\hbar^2}</math>
We end up getting:
<math>{\small^+_-} e^{-2ak}=2bk-1</math>, where <math>b=\frac{\hbar^2}{2m\alpha}</math>
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