Understanding Wave Function Probabilities for a Free Particle

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Discussion Overview

The discussion revolves around the wave function for a free particle with a known momentum, specifically addressing the interpretation of the wave function given as Asin(kx) and its implications for probability density along the x-axis. Participants explore the mathematical properties of wave functions, normalization conditions, and the conceptual understanding of probability in quantum mechanics.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions how the probability can be constant if the square of the wave function Asin(kx) is not a constant.
  • Another participant asserts that the correct wave function for a free particle is exp(i k x) and that the probability density is derived from the squared modulus of this complex function.
  • Concerns are raised about the physical realizability of the wave function Asin(kx), with some participants stating it cannot be normalized.
  • Discussion includes the distinction between a particle's position and the result of a measurement, with some participants suggesting that terminology reflects a deeper understanding of quantum mechanics.
  • Participants discuss the implications of the modulus and modulus squared of the wave function, with some clarifying that a constant modulus does not represent a viable wave function.
  • There is a mention of a later edition of the textbook that corrects previous misunderstandings regarding wave functions.
  • Some participants express a need to understand complex conjugates and their role in the context of wave functions.

Areas of Agreement / Disagreement

Participants express disagreement regarding the correctness of the wave function presented in the textbook, with some asserting it is incorrect while others defend its interpretation. The discussion remains unresolved on whether the textbook's explanation is fundamentally flawed or if it is a matter of misinterpretation.

Contextual Notes

Participants highlight limitations in the textbook's treatment of wave functions, particularly regarding normalization and the distinction between probability distributions and measurement outcomes. There is also a recognition that the terminology used may affect understanding.

Who May Find This Useful

This discussion may be useful for students and enthusiasts of quantum mechanics seeking to understand wave functions, probability densities, and the nuances of quantum measurement theory.

jjson775
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TL;DR
Location of a free particle with known momentum
The textbook I am self studying says that the wave function for a free particle with a known momentum, on the x axis, can be given as Asin(kx) and that the particle has an equal probability of being at any point along the x axis. I understand the square of the wave function to be the probability of finding the particle at a particular location. The square of Asin (kx) is not a constant so how can the probability be the same for all values of x? What am I missing?
 
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jjson775 said:
The textbook I am self studying
Which textbook?
 
jjson775 said:
The textbook I am self studying says that the wave function for a free particle with a known momentum, on the x axis, can be given as Asin(kx)
This is not correct. The correct function is ##\exp(i k x)##. The probability (more precisely the probability density) is the squared modulus of this complex function times an appropriate normalization factor, which is of course a constant, independent of ##x##.

If you can give the specific textbook and the specific chapter/page reference, we can check to see whether the textbook itself is wrong or whether you are misinterpreting something it said.
 
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jjson775 said:
Summary: Location of a free particle with known momentum

The textbook I am self studying says that the wave function for a free particle with a known momentum, on the x axis, can be given as Asin(kx) and that the particle has an equal probability of being at any point along the x axis. I understand the square of the wave function to be the probability of finding the particle at a particular location. The square of Asin (kx) is not a constant so how can the probability be the same for all values of x? What am I missing?
Moreover, such a wave-function is not physically realizable. The wave-function cannot be normalized.

Also, the modulus squared of the wave-function gives the probability distribution for the result of a measurement of position. It is not a probability distribution for where the particle is. A particle isn't anywhere until it is measured.
 
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PeterDonis said:
This is not correct. The correct function is ##\exp(i k x)##. The probability (more precisely the probability density) is the squared modulus of this complex function times an appropriate normalization factor, which is of course a constant, independent of ##x##.

If you can give the specific textbook and the specific chapter/page reference, we can check to see whether the textbook itself is wrong or whether you are misinterpreting something it said.

Serway Beichner Physics for Scientists and engineers, 5th edition, 2000, p. 1331.
See photo. An old book but I am old, too, an 80 year old retired engineer loving modern physics.
 

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jjson775 said:
Serway Beichner Physics for Scientists and engineers, 5th edition, 2000, p. 1331.
See photo. An old book but I am old, too, an 80 year old retired engineer loving modern physics.
The author does seem to have got confused between de Broglie waves and wave-functions (i.e. solutions to the Schrödinger equation). And, in particular, ##\psi(x) = A \sin(kx)## does not have the property he claims of a constant modulus squared.
 
PS the author seems to be a little half-hearted about QM. It may be a minor point, but if you really commit to a QM view of nature, then you stop saying "where the particle is" and start saying "the result of a measurement of the particle's position". Failing to make this linguistic change shows a luke-warm approach to QM, IMHO.
 
I understand your valid point. Maybe the wording changed in a later edition.
 
8th2010.PNG


In the eight edition of 2010, the whole section is rewritten and corrected (see 41.4 in the capture from page 1221).
 
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  • #10
Just forget this non-sensical book!
 
  • #11
It’s not just the book. I need to learn about complex conjugates.
 
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  • #12
Thread closed temporarily for Moderation...
 
  • #13
After some cleanup of a sub-thread about an error in a post, the thread is reopened. Thanks for your patience. :smile:
 
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  • #14
Again, I want to see how the probability density of a free particle on the x-axis with a known momentum is a constant. Is this right?
 

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  • #15
Technically it should be ##|A|^2## unless you assume that ##A## is a real number.
 
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  • #16
PeroK said:
Technically it should be ##|A|^2## unless you assume that ##A## is a real number.
Thanks. At my level of understanding, that was my assumption.
 
  • #17
jjson775 said:
Thanks. At my level of understanding, that was my assumption.
Note also that a function with a constant modulus is not a viable (physically realisable) wavefunction. That's an important point.
 
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  • #18
PeroK said:
Note also that a function with a constant modulus is not a viable (physically realisable) wavefunction. That's an important point.
Do you mean the modulus squared?
 
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  • #19
jjson775 said:
Do you mean the modulus squared?
The modulus is constant if and only if the modulus squared is constant.
 
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  • #20
In my simplified case the modulus is not a constant (varies with x) but the modulus squared is a constant, so does that mean the wave function is viable?
 
  • #21
jjson775 said:
In my simplified case the modulus is not a constant
Yes, it is. Only the phase (the ##\exp (i k x)## part) varies with ##x##.
 
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  • #22
jjson775 said:
In my simplified case the modulus is not a constant (varies with x) but the modulus squared is a constant, so does that mean the wave function is viable?
The modulus of your function is ##|A|## and the modulus squared is ##|A|^2##. Both are constant.
 
  • #23
PeterDonis said:
Yes, it is. Only the phase (the ##\exp (i k x)## part) varies with ##x##.
I‘m not familiar with this terminology but am familiar with the sinusoidal wave equation and the Euler formula. If the exp term is the phase part, what do you call “A” in the wave function?
 
  • #24
PeroK said:
The modulus of your function is ##|A|## and the modulus squared is ##|A|^2##. Both are constant.
I would like to test my understanding of these points:

1. The modulus (absolute value) of the wave function is irrelevant except in terms of being the square root of the modulus squared.
2. in this simple case, the wave function is not physically viable because it does not meet the normalization condition.
 

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  • #25
jjson775 said:
If the exp term is the phase part, what do you call “A” in the wave function?
Either the "amplitude" or the "modulus".
 
  • #26
Got it. Thanks
 

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