If we have a potential of the form $V(x,y)=k_{x}x^{2}+k_{y}y^{2}$ then that potential looks like this:
As you can see, this potential is clearly round. When dealing with simple harmonic oscillators (like a pendulum free to swing in 2 directions for small swings) then the behaviour we see is clearly... rounded. What I think I mean by this is if $k_x = k_y$ that the SHO in question needs more energy to reach somewhere based only on the euclidean distance from the equilibrium point and if they are different it's only a question of scaling the dimensions first.
Why is it then, that when I render out the 2D QHO what I get is decidedly rectangular.
This rendering uses hue for argument and brightness for magnitude.
Since it is possible I am using the wrong approach I will say that the eigenstates I am using are $\Psi_{n_x,n_y}(x,y,t)=X(x)\cdot Y(y)\cdot \phi(t)$ where $X$ and $Y$ are only different in their variables and values of k but are of the form $$\psi_{n}(\sqrt{\alpha}x) = \left(\frac{\alpha}{\pi}\right)^{1/4} \cdot \frac{1}{\sqrt{2^{n}n!}}\cdot H_{n}(\sqrt{\alpha}x) e^{-\frac{\alpha x^{2}}{2}}$$ And $\alpha = \sqrt{\frac{mk}{\hbar^{2}}}$ and $\phi(t)=e^{-itE/\hbar}$
From what I've read it seems like this should behave as though it had the potential described but for any values of k that I tried and for any superposition of states I could think of it still ends up looking rectangular.
Is this what I should expect? If so then why is the quantum case so different? Is my code wrong? If so where in my reasoning is the misstep?