Momentum eigenfunctions proof and Fourier Transform question

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Discussion Overview

The discussion revolves around the definitions and properties of momentum eigenfunctions and operators in quantum mechanics, specifically focusing on the operator ##\Psi## and its relation to Fourier transforms. Participants explore the implications of these definitions and their representations in different spaces, addressing both conceptual and technical aspects of the topic.

Discussion Character

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

Main Points Raised

  • Some participants question how the operator ##\Psi## is defined and whether its definition affects the validity of related concepts.
  • Others clarify that the expressions discussed represent eigenfunctions of different operators and are not related by Fourier transformation.
  • There is a discussion about the significance of subscripts in the functions ##\psi_{\mathbf{k}}(\mathbf{r})## and ##\phi_{\mathbf{r}}(\mathbf{k})##, indicating that they represent different states compared to ##\psi## and ##\phi## without subscripts.
  • One participant notes that while ##\psi(\mathbf{r})## and ##\phi(\mathbf{k})## are related through Fourier transform, the other functions are not, as they correspond to eigenfunctions of different operators.
  • A question is raised regarding the difference in signs in the exponents of the functions ##\Psi_k## and ##\Phi_r##, prompting further exploration of their definitions and implications.

Areas of Agreement / Disagreement

Participants express differing views on the definitions and relationships of the operators and eigenfunctions discussed. There is no consensus on the implications of these definitions, and the discussion remains unresolved regarding the nature of the operator ##\Psi## and its properties.

Contextual Notes

Some participants express uncertainty about the material, indicating that they are beginners in quantum mechanics. This may affect their understanding and interpretation of the concepts discussed.

Joker93
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I have the following problem:
 

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How do you define the operator ##\Psi##?
 
DrDu said:
How do you define the operator ##\Psi##?
the equations are from this link

https://en.wikipedia.org/wiki/Position_and_momentum_spaceBut, is it a matter of how you define things? Isn't there a right way to do it that does not depend on how you define the operator? Excuse me if these questions are moronic, but I haven't been far into quantum mechanics yet(I am a self learner at this point).
 
I think you misunderstood the terms here. The first expression is the eigenfunction of momentum operator in position representation, and the second expression is the eigenfunction of position in momentum representation. They are not related by Fourier transformation.
 
Adam Landos said:
But, is it a matter of how you define things? Isn't there a right way to do it that does not depend on how you define the operator? Excuse me if these questions are moronic, but I haven't been far into quantum mechanics yet(I am a self learner at this point).
All I know from your post is that ##\Psi## apparently is an operator which has some eigenfunctions. So it seems appropriate to as for some more details before answering your questions.
 
blue_leaf77 said:
I think you misunderstood the terms here. The first expression is the eigenfunction of momentum operator in position representation, and the second expression is the eigenfunction of position in momentum representation. They are not related by Fourier transformation.
check this link by Wikipedia please

https://en.wikipedia.org/wiki/Position_and_momentum_space
 
DrDu said:
All I know from your post is that ##\Psi## apparently is an operator which has some eigenfunctions. So it seems appropriate to as for some more details before answering your questions.
its all in the Wikipedia link that I have provided you with.
 
Adam Landos said:
its all in the Wikipedia link that I have provided you with.
I can't find any operator ##\Psi## in this link.
 
DrDu said:
I can't find any operator ##\Psi## in this link.
I think its r(hat)=i*d/dk
its in the link under "Functions and operators in momentum space"
 
  • #10
You think so?!? So basically, we shall not only answer your question, but also guess what your question might be?
 
  • #11
DrDu said:
You think so?!? So basically, we shall not only answer your question, but also guess what your question might be?
I found it in the link(by Wikipedia) and I also have given you the link and told you where to look for it. I "think so" because I have not seen operators in my self-stude of quantum mechanics yet, I am a beginner as I warned you.
 
  • #12
DrDu said:
You think so?!? So basically, we shall not only answer your question, but also guess what your question might be?
in the link, it writes: "position operator r(hat)".
 
  • #13
Note the presence of subscripts in ##\psi_{\mathbf{k}}(\mathbf{r})## and ##\phi_{\mathbf{r}}(\mathbf{k})##, their presence give them different meaning from ##\psi## and ##\phi## without subscripts. It's true that ##\psi(\mathbf{r})## and ##\phi(\mathbf{k})## are related through Fourier transform, because both functions actually represent the same state, they are just represented in different space. On the other hand, ##\psi_{\mathbf{k}}(\mathbf{r})## and ##\phi_{\mathbf{r}}(\mathbf{k})## are not related through Fourier transform as they correspond to different state (more precisely because they are eigenfunctions of different operators).
Adam Landos said:
I am a beginner as I warned you
For beginners, Wikipedia and other online sources are often not very good resources to learn because they are generally not designed to initiate learning. It's advisable to start your adventure from standard textbooks.
 
  • #14
blue_leaf77 said:
Note the presence of subscripts in ##\psi_{\mathbf{k}}(\mathbf{r})## and ##\phi_{\mathbf{r}}(\mathbf{k})##, their presence give them different meaning from ##\psi## and ##\phi## without subscripts. It's true that ##\psi(\mathbf{r})## and ##\phi(\mathbf{k})## are related through Fourier transform, because both functions actually represent the same state, they are just represented in different space. On the other hand, ##\psi_{\mathbf{k}}(\mathbf{r})## and ##\phi_{\mathbf{r}}(\mathbf{k})## are not related through Fourier transform as they correspond to different state (more precisely because they are eigenfunctions of different operators).
yes, sorry for the misunderstanding.
But, why does Ψk have a plus sign on the exponent while Φr has a minus sign?
 
  • #15
Adam Landos said:
why does Ψk have a plus sign on the exponent while Φr has a minus sign?
##\psi_{\mathbf{k}}(\mathbf{r})## is an eigenfunction of momentum operator ##\hat{\mathbf{p}} = -i\hbar\frac{\partial}{\partial \mathbf{r}}##, so, to calculate ##\psi_{\mathbf{k}}(\mathbf{r})## you need to solve
$$
\mathbf{p} \psi_{\mathbf{k}}(\mathbf{r}) = -i\hbar\frac{\partial}{\partial \mathbf{r}} \psi_{\mathbf{k}}(\mathbf{r})
$$
 

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