I am solving the Schrödinger equation for a particle in a hybrid system. Specifically I have to solve the following differential equation
$$ - \frac{\hbar^2}{2}\frac{d}{dx}\left(\frac{1}{m^{*}(x)}\frac{d\psi}{dx}\right) -\frac{\hbar^2}{2m^{*}(x)} \frac{d^2\psi}{dy^2} + V(x)\psi = E\psi \ \ \ \tag{1} $$
I would like to know: Is this problem separable? I.e. can the solutions be written as $\psi(x,y)=\Phi(x)\chi(y)$?
To investigate this question, I plugged the separable solution into (1) and found after some rearrangement:
$$ \frac{1}{\chi(y)}\frac{d^2\chi(y)}{dy^2} + \frac{m^{*}(x)}{\Phi(x)} \cdot \frac{d}{dx}\left(\frac{1}{m^{*}(x)}\frac{d\Phi}{dx}\right) + 2m^{*}(x) \cdot \frac{V(x)-E}{\hbar^2} = 0 $$
Now, the first term depends only on y while the two other terms depend only on x. Therefore one can separate the above into two differential equations, a simple one for $\chi(y)$ and a nasty one for $\Phi(x)$. Does this prove that the solutions of (1) are separable? And say they are, how would I go about calculating the solutions to the differential equation for $\Phi(x)$. The spatial dependence of the mass $m^{*}(x)$ is rather annoying.