Question about Uncertainty Principle

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Discussion Overview

The discussion revolves around the uncertainty principle in quantum mechanics, specifically in the context of the Infinite Square Well problem. Participants explore the relationship between energy eigenstates and momentum uncertainty, questioning how momentum uncertainty varies across different energy states despite having two possible momentum outcomes.

Discussion Character

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

Main Points Raised

  • One participant notes that an energy eigenstate in the Infinite Square Well is in an equal superposition of two momentum eigenstates with opposite signs, leading to two possible outcomes for momentum measurements.
  • Another participant questions the expression for momentum uncertainty in terms of expectation values, suggesting that while

    =0, is not zero, leading to confusion about the intuition behind increased momentum uncertainty in higher energy eigenstates.

  • A participant argues that the question is misleading because, in the Infinite Square Well, a momentum operator cannot be defined, which complicates the concept of momentum uncertainty.
  • Some participants discuss the implications of having two opposite momentum values and how the uncertainty might increase with higher energy due to the larger gap between positive and negative momentum values.
  • One participant uses an analogy involving expected payments to illustrate how variance can differ even with the same average, questioning the intuitive understanding of uncertainty in quantum mechanics.
  • There is a discussion about the necessity for operators representing observables to be Hermitian or self-adjoint, with questions raised about the differences between these terms and how to identify non-Hermitian operators.

Areas of Agreement / Disagreement

Participants express differing views on the definition and implications of the momentum operator in the context of the Infinite Square Well, with some asserting that it cannot be defined while others challenge that notion. The discussion remains unresolved regarding the intuition behind momentum uncertainty and the conditions under which it varies.

Contextual Notes

Limitations include the lack of consensus on the definition of the momentum operator in the Infinite Square Well and the implications of using non-Hermitian operators in quantum mechanics. There are also unresolved questions about the intuitive understanding of uncertainty and variance in quantum measurements.

Who May Find This Useful

This discussion may be of interest to students and enthusiasts of quantum mechanics, particularly those exploring the concepts of uncertainty, eigenstates, and the mathematical foundations of quantum operators.

Joker93
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In the Infinite Square Well problem, an energy eigenstate is in an equal superposition of two momentum eigenstates with eigenvalues that are opposite in sign(like standing waves that are formed by two wavefunctions corresponding to "opposite momentums").
So, for every energy eigenstate, we always have two possible outcomes for the momentum in a momentum measurement.
So, the question is, why does the uncertainty in the momentum change(increase) for different energy eigenstates if each eigenstate has exactly two outcomes?
Thanks in advance!
 
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What is an expression for momentum uncertainty in terms of expectation values?
 
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Since in the infinite-wall example you cannot define a momentum operator and thus no momentum uncertainty the question is misleading to begin with. It's an important exercise to figure out that for this geometry no self-adjoint operator that generates translations exists! Look for the topic in this forum. I've once posted a discussion on it.
 
George Jones said:
What is an expression for momentum uncertainty in terms of expectation values?
<p^2>-<p>^2. So, two opposite in sign momentums give <p>=0 but not <p^2>=0. But again, i can't quite get the intuition behind being more uncertain about the momentum in eigenstates of higher energy. Mathematically, i understand it in the way i explained it. But the intuition is unclear for me. We always have two possible values of momentum.
 
vanhees71 said:
Since in the infinite-wall example you cannot define a momentum operator and thus no momentum uncertainty the question is misleading to begin with. It's an important exercise to figure out that for this geometry no self-adjoint operator that generates translations exists! Look for the topic in this forum. I've once posted a discussion on it.
What do you mean by you can't define a momentum operator? Can't we act on a wavefunction with the momentum operator in just the same way as in any other problem? We can also find the expectation value of the momentum. I am feeling that i am getting something fundamental wrong and that's a bad thing! Help, SOS! :D
 
The higher the energy the greater the momentum. Since you don't know which direction the particle is traveling in there is more uncertainty due to the bigger gap between +p and -p.
 
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Adam Landos said:
<p^2>-<p>^2. So, two opposite in sign momentums give <p>=0 but not <p^2>=0. But again, i can't quite get the intuition behind being more uncertain about the momentum in eigenstates of higher energy. Mathematically, i understand it in the way i explained it. But the intuition is unclear for me. We always have two possible values of momentum.

Suppose you had a job and you knew that next week you would be paid either $99 or $101. Well, the average is $100 and there is some uncertainty.

Suppose you knew that next week you would be paid either $50 or $150? The average is still $100 and you still have only two possible values.

Would you say that the "uncertainty" (technically, it's the "variance" we should be talking about) is more, less or the same in the second case?

On a more general point, you are going to run into all sorts of problems in physics if you start with a priori "intuitive" ideas about what certain words mean. For example, the term "expected" value in stats and QM is not really a good word. It really should be the "mean" value. The "expected value" for the roll of a die is 3.5, which is, of course, an impossible outcome.

Words (and your a priori expectations of what you think they should mean) will lead you astray, where the maths and the mathematical definition of those words will not.
 
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Adam Landos said:
What do you mean by you can't define a momentum operator? Can't we act on a wavefunction with the momentum operator in just the same way as in any other problem? We can also find the expectation value of the momentum. I am feeling that i am getting something fundamental wrong and that's a bad thing! Help, SOS! :D

For a short answer, see

https://www.physicsforums.com/threads/particle-in-a-box-in-momentum-basis.694158/#post-4398736

For the mathematical details, see

http://arxiv.org/abs/quant-ph/0103153v1
 
vanhees71 said:
Wow, lot's of great stuff there! As a beginner on QM, i find these to be very enlightening and subtle!
But, i have one more question. In order for an observable to be attributed to an operator, the operator must be Hermitian or self-adjoint and why? Also, what is their difference? Because there is a lot of confusion among people.
Also, how to detect if an operator is not a good one(not self-adjoint or not Hermitian) in a problem(or in general)?
 
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George Jones said:
What is an expression for momentum uncertainty in terms of expectation values?

vanhees71 said:
For the mathematical details, see

http://arxiv.org/abs/quant-ph/0103153v1

Mea culpa! I was more careful in

George Jones said:
I think this is a bit subtle. What is the momentum operator for the square well? See

http://arxiv.org/abs/quant-ph/0103153.

Adam Landos said:
what is their difference? Because there is a lot of confusion among people.?

I don't think that there is a completely standard usage of the term "Hermitian"; see the discussion at

https://www.physicsforums.com/threa...bles-are-hermitian.728302/page-2#post-4605707
 
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