Proving sum rule for position matrix elements in quantum mechanics

Join the discussion
Registration is free. Ask a follow-up in this thread, or start your own.
4 replies · 3K views
gulsen
Messages
215
Reaction score
0
[tex]\widehat{H} = \frac{p^2}{2m} + V(x)[/tex]

if eigenvalue of H operator is [tex]E_n[/tex] and eigenvectors are [tex]u_n[/tex], show that

[tex]\Sigma_m (E_m-E_n) |x_{mn}|^2 = \frac{\hbar^2}{2m}[/tex]

is true. here, [tex]x_{mn} = (u_m, xu_n)[/tex] is a matrix element.
 
Physics news on Phys.org
Could you please show us what you've done so far? We can't help until you do. Thanks.
 
well, we've read the question over and over again and, ummm, that's almost it i guess. expect we tried orthagonality relation -maybe it had something with the question- and realized we've all messed it up...

in short, we couldn't manage to get anything worth to mention...
 
I don't understand your question. Is that sum supposed to be over n and m? And what exactly is xmn? Is it a vector? A complex number? What does x represent? Please be clearer with your notation.
 
gulsen,

Here are some thoughts to help you get started. The first thing I would do is expand out the left hand side so you can see the structure. In other words, write it something like [tex]\sum_m (E_m - E_n)\langle n | x | m \rangle \langle m | x | n \rangle,[/tex] where all I have done is make everything very explicit. From this expression is should be clear that you can perform the m sum, so why don't you try again with this hint.

StatusX.

The sum is just over m, it just so happens that the result is independent of n. Also, [tex]x_{n m} = \langle n | x | m \rangle[/tex] is a matrix element (a complex number) of the position operator [tex]x[/tex].