Average value in superposition question

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Discussion Overview

The discussion revolves around the calculation of average values, specifically energy and position, for a particle in a superposition of states in quantum mechanics. Participants explore the implications of using different summation indices in these calculations and the role of orthogonality of eigenfunctions.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions why different summation indices (n, m) are used when calculating average values for a particle in superposition.
  • Another participant explains that using the same summation index would result in missing mixed terms, referencing the orthogonality of eigenfunctions.
  • There is a discussion about the implications of orthogonality on the calculation of average position versus energy, highlighting that energy yields eigenvalues while position does not.
  • Participants express uncertainty about the physical meaning of mixed terms (A12, A21) in relation to energy and position calculations.
  • One participant emphasizes the mathematical reasoning behind using different indices, noting that it prevents the loss of mixed terms when multiplying sums.
  • Another participant mentions that terms involving c1c2 are significant in calculating probabilities and interference effects.

Areas of Agreement / Disagreement

Participants generally agree on the mathematical reasoning behind using different summation indices, but there remains uncertainty regarding the physical implications of these terms and their roles in different observable calculations.

Contextual Notes

Participants highlight the distinction between quantized energy and non-quantized position, as well as the importance of orthogonality in the context of quantum mechanics. The discussion does not resolve the deeper physical meanings of the mixed terms.

Alexitron
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Hi there.
A quick question: When calculating the average energy (or any value) of a particle which is in superposition, why the sums have different summation index (n,m)?

Thanks!
 

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If you multiply a number a=a1+a2 with itself, you get a1² + a2² + 2a1a2. If you take the same summation index for both sums in your problem, you end up only with terms an² and don't get the mixed terms.

/edit: You may be wondering why in the end, you actually don't get the mixed terms. But remember that this is due to the orthogonality ψnψmnm of the eigenfunctions of the (hermitian) Hamiltonian. This is not true for arbitrary sums of wavefunctions.
 
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Thanks a lot for your reply.
it bothers me for some time

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.
 
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.
Yes. But you do understand why it is mathematically wrong to use the same summation index, don't you?
 
kith said:
Yes. But you do understand why it is mathematically wrong to use the same summation index, don't you?
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)?
Sorry for asking such trivial things, but I'm stuck here.

I mean what's wrong with the following?
 

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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.
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:
And what's the physical meaning of A12 and A21 that energy doesn't have (I know why energy doesn't have them)?
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.

Terms c1c2 do play a role when you calculate probabilities instead of average values. They are responsible for interference (see the double slit for example).

/edit: Your second calculation only yields the same result because ψn is an eigenvector to H. Else you would get Ʃn|cn|² * I, where I stands for the numerical value of the integral. In general, this is not the same as Ʃn,mcn*cm.
 
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Thanks for your time. You helped me a lot to figure it out.
 

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