Infinite or undefined standard deviation in HUP

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Discussion Overview

The discussion revolves around the implications of the Heisenberg Uncertainty Principle (HUP) on the standard deviation of conjugate variables, particularly in the context of potential limits on measurements such as momentum and energy. Participants explore theoretical scenarios and the nature of canonical conjugate observables, questioning the implications of precision in measurement and the existence of limits in physical quantities.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • One participant suggests that if one conjugate variable's standard deviation is zero, the other must have an infinite or undefined standard deviation, questioning the implications when limits on the other variable exist.
  • Another participant asserts that canonically conjugate observables have all real numbers in their spectrum, indicating they are unbounded and lack limits.
  • A participant raises a hypothetical scenario regarding the momentum of a particle at a precise point, suggesting that beyond a certain momentum, the particle's mass-energy could lead to a black hole, thus questioning the infinite nature of the momentum spectrum.
  • Another participant points out that canonical commutation rules for interacting particles are valid only in flat space-time, which excludes scenarios involving black holes.
  • One participant acknowledges a flaw in their reasoning regarding virtual particles and their dynamics, indicating a lack of understanding of their implications.
  • Another participant expresses gratitude for insights shared and reflects on the complexity of the topic, particularly in relation to uncertainty relations in curved space-time.

Areas of Agreement / Disagreement

Participants express differing views on the nature of conjugate variables and the implications of measurement precision, with no consensus reached on the existence of limits or the nature of virtual particles.

Contextual Notes

Participants acknowledge limitations in their understanding of the implications of the HUP, particularly in complex scenarios involving black holes and curved space-time, which may affect the validity of their arguments.

nomadreid
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If we measure one conjugate variable in an uncertainty relation precisely , i.e., so its standard deviation is zero, then by the HUP the sd of the other one is either infinite or undefined. But what about the cases when the other conjugate variable has limits: e.g., there cannot be an infinite spread for momentum or energy? Is it then better to just say that the spread is undefined in this case?
 
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Canonically conjugate observables always have all reals in the spectrum, hence are unbounded and have no limits.
 
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A. Neumaier said:
Canonically conjugate observables always have all reals in the spectrum, hence are unbounded and have no limits.
OK. This raises the (certainly naïve) question: suppose we refer to the momentum of particle at a determined point. Since the point is precise, you have the infinite spectrum of momentum. However, beyond a certain momentum the particle has enough mass-energy at that point you end up with a black hole, making the point lose its exact value, which would mean that the spectrum of the momentum would not be able to go beyond that limit. Hence not infinite. There is obviously a basic flaw in my reasoning here, but what?
 
nomadreid said:
OK. This raises the (certainly naïve) question: suppose we refer to the momentum of particle at a determined point. Since the point is precise, you have the infinite spectrum of momentum. However, beyond a certain momentum the particle has enough mass-energy at that point you end up with a black hole, making the point lose its exact value, which would mean that the spectrum of the momentum would not be able to go beyond that limit. Hence not infinite. There is obviously a basic flaw in my reasoning here, but what?
Canonical commutation rules for interacting particles are valid in flat space-time only. This excludes black holes.
 
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Ah, I overlooked that. Excellent point, thank you, A.Neumaier. That probably takes care of my other counterexamples. No superluminary virtual particles, then?
 
Thank you, A.Neumaier, for that answer and the excellent link; my delay in answering was due to my reading through it. (I had a feeling I shouldn't have used the concept "virtual particles"...) Very interesting and well written, and there are a few things there that I intend to try to understand more thoroughly in the course of time.
(Wikipedia is a suitable target -- even in secondary school assignments, Wikipedia is not accepted as a reliable source due to the fact that the articles are not signed.) I was also trying to find out (online) what corresponds to the Uncertainty Relations (i.e., the canonical commutation rules) in curved space-time, but the discussions I found exceed my present level in the subject.
 

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