Yes. But you do understand why it is mathematically wrong to use the same summation index, don't you?Alexitron said:So for example,(ψ=c1ψ1 + c2ψ2) when calculating the average position (or any other Item A) of a particle, if we had the same summation index we wouldn't have the terms X_12 and X_21. But when we calculate the energy we don't have these mixed (E_12,E_21) terms but eigenvalues (E_1,E_2) due to orthogonality.
Well, i know how the values of <x> and <E> are calculated and that energy is quantized but the position for example is not , but to be honest i don't understand why the conjugate ψ* has different index. The only thing i can think is that we lose the factors A12 and A21 when calculating <A> (what you said in your previous reply). Is that the reason? And what's the physical meaning of A12 and A21 that energy doesn't have (I know why energy doesn't have them)?kith said:Yes. But you do understand why it is mathematically wrong to use the same summation index, don't you?
Forget about QM for a moment and think purely mathematical. ψ is a complex number which can be written as a sum Ʃnψn, and so is ψ*. If you multiply two sums, you can't use the same index because this doesn't yield any mixed terms.Alexitron said:Well, i know how the values of <x> and <E> are calculated and that energy is quantized but the position for example is not (of course for t≠0), but to be honest i don't understand why the conjugate ψ* has different index.
Actually, there's nothing specific to energy here. ψ can be decomposed in an orthogonal set of eigenvectors to any observable, so <A> = Ʃn|cn|²an is the result for the average value of an arbitrary observable A.Alexitron said:And what's the physical meaning of A12 and A21 that energy doesn't have (I know why energy doesn't have them)?