- #1
Ernesto Paas
- 5
- 0
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: [tex]\sum_{n,m} \langle n | b_{n}^* \, \hat{A} \, c_{m} | m \rangle [/tex]
And what's to stop me from moving the operator to the left and getting a kronecker-delta?
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: [tex]\sum_{n,m} \langle n | b_{n}^* \, \hat{A} \, c_{m} | m \rangle [/tex]
And what's to stop me from moving the operator to the left and getting a kronecker-delta?