I When can one clear the operator

Ernesto Paas
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Hi all!
I'm having problems understanding the operator algebra. Particularly in this case:
Suppose I have this projection ## \langle \Phi_{1} | \hat{A} | \Phi_{2} \rangle ## where the ##\phi's ## have an orthonormal countable basis.
If I do a state expansion on both sides then I suppose I'd get this: \sum_{n,m} \langle n | b_{n}^* \, \hat{A} \, c_{m} | m \rangle
And what's to stop me from moving the operator to the left and getting a kronecker-delta?
 
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I presume your expansion states are eigenstates of ##\hat A##? If so, then I'd say "yes..."
 
strangerep said:
I presume your expansion states are eigenstates of ##\hat A##? If so, then I'd say "yes..."
Ah no... Sorry for not pointing that out. They are just of the same same arbitrary orthonormal basis.
 
Oh, well, if your expansion states are not eigenstates of ##\hat A##, then... what are they? E.g., what is $$\hat A |m\rangle ~=~ ?$$
 
I don't know, that's the problem. I've seen bras and kets being moved around without being eigenstates of an operator. Like in this case $$ \langle a | b \rangle \langle c1 | A | c2 \rangle \langle d | e \rangle = \langle a | b \rangle \langle d | e \rangle \langle c1 | A | c2 \rangle $$
 
Is the operator like glued to the left ket? Can I move the bra around?
 
Think of the bra ##\langle a|## as a row vector "##a^T##'', the ket ##|b\rangle## as a column vector "##b##", and the operator ##\hat A## as a matrix ##A##. I'll write it the overall expression as ##a^T A b##. Does that much make sense?
(I'm not sure how much ordinary linear algebra you already know.)
 
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Ok it hadn't occurred to me to think of them in that way. It wouldn't make sense to do a commutation there if the rows didn't equal the columns. Nevertheless, moving scalars around wouldn't be a problem.

Thanks, it was actually really easy...
 
More generally, see the second line of my signature below... :oldbiggrin:

Ballentine, ch1, can help a lot with these sort of questions.
 
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