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Homework Statement
Find the energy eigenvalues and eigenfunctions for the one-dimensional infinite square well. Calculate the matrices for the position and momentum operators, Q and P, using these eigenfunctions as a basis.
Homework Equations
The energy eigenvalues are
[tex]E_n = \frac{\pi^2 \hbar^2}{2Ma^2}n^2[/tex]
and the eigenfunctions are,
[tex]\psi_n(x) = \sqrt{\frac{2}{a}} sin \left ( \frac{n \pi}{a} x \right ) [/tex]
The Attempt at a Solution
Finding the energy eigenvalues and eigenfunctions is straightforward. What is really confusing me is how to use the eigenfunctions as a basis to find the matrix representations of these operators. This is problem 4.2 in Ballentine's Quantum Mechanics, and I can't find any useful information in the chapter for doing this sort of problem. Here is the best attempt I have:
The position operator Q satisfies,
[tex]\hat Q \psi_n(x) = x_n \psi_n(x)[/tex]
If we represent [itex]\psi[/itex] as a column matrix, we can write:
[tex]\psi_n(x) = \left[ \begin{array}{c} \psi_1(x) \\ \psi_2(x) \\ \vdots \\ \psi_n(x) \end{array} \right][/tex]
Using this representation,
[tex] \hat Q \left[ \begin{array}{c} \psi_1(x) \\ \psi_2(x) \\ \vdots \\ \psi_n(x) \end{array} \right] = \left[ \begin{array}{c} x_1 \psi_1(x) \\ x_2 \psi_2(x) \\ \vdots \\ x_n \psi_n(x) \end{array} \right]= \left[ \begin{array}{cccc} x_1 & 0 & \hdots & 0\\ 0 & x_2 & 0 \hdots & 0 \\ \vdots & \vdots & \ddots & \vdots \\ 0 & 0 & 0 & x_n \end{array} \right] \left[ \begin{array}{c} \psi_1(x) \\ \psi_2(x) \\ \vdots \\ \psi_n(x) \end{array} \right] [/tex]
So Q would be this matrix with the x's along the diagonal:
[tex] \hat Q = \left[ \begin{array}{cccc} x_1 & 0 & \hdots & 0\\ 0 & x_2 & 0 \hdots & 0 \\ \vdots & \vdots & \ddots & \vdots \\ 0 & 0 & 0 & x_n \end{array} \right] [/tex]
I feel like the answer is supposed to be more specific than this
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