Time-energy uncertainty (question after reading FAQ)

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Discussion Overview

The discussion revolves around the time-energy uncertainty principle in quantum mechanics, particularly focusing on the implications of energy measurements and the nature of quantum states during such measurements. Participants explore the relationship between energy eigenstates and superpositions, questioning how measurements yield results that may not correspond exactly to discrete energy eigenvalues.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Mike questions why a measurement yielding an energy close to an eigenvalue suggests averaging over states rather than selecting a discrete energy eigenstate.
  • One participant notes that real measurements are not "pure" and require finite time, implying that results can vary and are expressed as superpositions of energy eigenstates.
  • Another participant asks what energy corresponds to if it does not match any energy eigenstate, raising the question of whether superpositions have defined energies.
  • There is a discussion about whether a measurement of energy must result in an energy eigenstate, with some suggesting that finite-duration measurements yield states with energies roughly corresponding to eigenstates.
  • Further clarification is sought on the nature of energy measurements, with a participant asserting that no perfect energy measurement exists, and that longer measurements may lead to the discounting of certain energy eigenstates.

Areas of Agreement / Disagreement

Participants express confusion and differing views on the implications of energy measurements and the nature of quantum states. There is no consensus on whether measurements must yield energy eigenstates or how superpositions relate to measured energies.

Contextual Notes

Participants highlight the limitations of finite measurement times and the complexities involved in defining the relationship between measured energies and energy eigenstates. The discussion reflects unresolved questions about the nature of quantum measurements.

mikeph
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Hi,
The FAQ is a good answer, but it leaves me wondering about something.

From what I read, the jist is that a short enough measurement sees no difference between an energy eigenstate and a quantum superposition which mostly comprises of that energy eigenstate but also has a few other components from other eigenstates in there.

But when we make a measurement and get, say an off-centre energy E + dE, what does that mean? Why is the molecule not choosing between all the possible discrete energies based on the probability factors c1, c2..., and returning one of these? The fact that we actually measure an energy very close to but not equal to the energy eigenvalue implies (to me) that somehow we're averaging the energies of all the states with the weighting factors. I don't understand why an average is being taken, if we make an energy measurement then the molecule is forced into an energy eigenstate, and we get an exact energy.

The uncertainty about the initial state is then removed, and our measurement is an energy distribution, but the distribution is discrete amongst the energy eigenstates, not just a smearing around the state with the largest weighting.

Thanks for any help
Mike
 
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MikeyW said:
I don't understand why an average is being taken, if we make an energy measurement then the molecule is forced into an energy eigenstate, and we get an exact energy.
Well, real measurements are never "pure" energy measurements, or need infinite time for that.

With a finite measurement time, the result can be "anything". You can express this as superposition of energy eigenstates, but that is just a mathematical calculation - you can express every state as such a superposition.
 
But we are extracting a real amount of energy out. If that energy does not correspond to any of the energy eigenstates, then what does it correspond to? Does a superposition of these states still have an energy?
 
Particles don't have to be in energy eigenstates, where is the problem?
Does a superposition of these states still have an energy?
Sure
 
So when we make a measurement of energy, the result doesn't have to be an energy eigenstate because the final state isn't necessarily in that state? Can you see why I'm a bit confused by this idea, it seems to contradict the idea that an energy measurement fixes the state to one of definite energy.

Would a more accurate expression of that statement ^^ be that a finite-duration energy measurement fixes the state to one with roughly the same energy as an energy eigenstate? And the longer you measure it, the more of the other energy eigenstates go out of phase and can be discounted from the measurement?
 
MikeyW said:
So when we make a measurement of energy
As I said, there is no perfect energy measurement. There are very good approximations, however.
, the result doesn't have to be an energy eigenstate because the final state isn't necessarily in that state? Can you see why I'm a bit confused by this idea, it seems to contradict the idea that an energy measurement fixes the state to one of definite energy.
In the limit of a perfect energy measurement.
Would a more accurate expression of that statement ^^ be that a finite-duration energy measurement fixes the state to one with roughly the same energy as an energy eigenstate? And the longer you measure it, the more of the other energy eigenstates go out of phase and can be discounted from the measurement?
Right
 

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