In an expansion around the point \(z=1\), the recurrence relation is: \[a_{n+1}=\frac{1}{n+1}\, a_n\]
Consider the differential equation \(y^{\prime\prime} - 2y^{\prime} + y = 0\).
The eigenstates for a quantum mechanical particle inside a 2-dimensional infinite potential well located between \(x=0\) and \(L_x\) and \(y=0\) and \(L_y\) are: \[\left|{n_x,n_y}\right\rangle \doteq \sqrt{\frac{2}{L_x}}\sin{\frac{n_x\pi x}{L_x}} \sqrt{\frac{2}{L_y}}\sin{\frac{n_y\pi y}{L_y}}\]
At \(t=0\), the system is in an initial state:
\[\psi(x,y,0)= \sqrt{\frac{30}{L_x^5 L_y^5}}(L_x x-x^2)(L_y y-y^2)\]
Find an exact expression for the wave function as a function of time.
Fun Extension: Plot an approximation for the probability density at \(t=0\) and at an interesting later time.