fluidistic
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Homework Statement
Show that for a unidimensional potential of the form V(x)=v(-x), the solutions to the time independent Schrödinger's equation have a defined parity as long as these solutions does not correspond to eigenvalues not degenerated.
Homework Equations
-\frac{\hbar ^2}{2m} \cdot \frac{\partial ^2 \Psi}{\partial x^2}+V(x) \Psi =E\Psi.
The Attempt at a Solution
My idea: replace V(x) by V(-x) in the equation I just gave and then find \Psi. Then show that \Psi is either odd or even.
I have no idea about the non degenerated eigenvalues of \Psi...
I'm stuck on starting to solve the equation. I'm a bit familiar with differential equations but not with partial ones.
Is it an equation of the form c_1y''+gy=c_2y where y=\Psi and g=V(-x)? I realize I've no idea why I even bothered changing V(x) for V(-x).
I don't really know what to do. I'd like a little push.