Position measurement in Non-Relativistic QM

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Discussion Overview

The discussion revolves around the concept of position measurement in non-relativistic quantum mechanics (NR-QM), particularly the implications of measuring position with exact precision and the associated challenges regarding momentum uncertainty and wave function collapse.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants assert that measuring position with exact precision leads to infinite momentum uncertainty, which raises questions about the validity of such measurements.
  • One participant suggests that wave function collapse is not necessary unless subsequent measurements are made, proposing that the measurement can be considered complete without collapse.
  • Another participant highlights that the collapse of the wave function can be subjective and does not necessarily have to conform to traditional eigenvector projections.
  • It is noted that a Dirac delta function, which represents perfect position measurement, is not a legitimate wave function within Hilbert space, complicating the notion of infinite precision.
  • Some participants propose that while infinite precision is unattainable, position can be measured with arbitrarily good finite precision, which may be practically sufficient.

Areas of Agreement / Disagreement

Participants express differing views on the feasibility of exact position measurement and the implications of wave function collapse, indicating that the discussion remains unresolved with multiple competing perspectives.

Contextual Notes

The discussion touches on the limitations of continuous variable measurements and the mathematical challenges associated with representing idealized states like the Dirac delta function within the framework of quantum mechanics.

andresB
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I've read several times in textbooks that in NR-QM you can measure with exact precision the position of a particle if you don't care at all for the momentum (because the uncertainty of the momentum will be infinite), it always seemed reasonable enough for me but now that I think about it, it should be impossible in principle because the wave function would collapse to a delta function, and the delta function is not in the hilbert space of the wave functions.

Any thoughts?
 
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The quick answer is that one doesn't need collapse unless one is doing another measurement after the first. So we can just declare the measurement done, and the particle destroyed after that.

However, the collapse rule is actually more general, and doesn't have to be a projection onto an eigenvector of the observable. The heuristic way to see this is that what you consider a measurement is subjective, so you can collapse it onto the eigenvector and rotate it, and call that process the measurement.

OK, but that still doesn't help with continuous variables, since the eigenvector itself is not a legitimate wave function. For continuous variables the collapse is defined by Eq 3 of http://arxiv.org/abs/0706.3526. Remarkably, Ozawa discovered that there is a measurement model that will give a sharp position measurement, which is summarized in section 2.3.2 of that paper.
 
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andresB said:
I've read several times in textbooks that in NR-QM you can measure with exact precision the position of a particle if you don't care at all for the momentum (because the uncertainty of the momentum will be infinite), it always seemed reasonable enough for me but now that I think about it, it should be impossible in principle because the wave function would collapse to a delta function, and the delta function is not in the hilbert space of the wave functions.

Any thoughts?
That means that you cannot measure position with infinite precision, but you can measure position with an arbitrarily good finite precision. For all practical purposes, this is the same.
 
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Demystifier said:
That means that you cannot measure position with infinite precision, but you can measure position with an arbitrarily good finite precision. For all practical purposes, this is the same.

This is seen by the fact a state with perfect position is a Dirac Delta Function - which isn't really a function, and certainly doesn't belong to a Hilbert space.

Thanks
Bill
 

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