What does it mean to find eigenvectors of some operator in some basis?

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Discussion Overview

The discussion revolves around the concept of finding eigenvectors of angular momentum operators (Lx, Ly, Lz) in quantum mechanics, specifically the significance of expressing these eigenvectors in the basis of another operator, such as Lz. Participants explore the implications of working in different bases and the process of diagonalization.

Discussion Character

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

Main Points Raised

  • One participant expresses confusion about the meaning of finding eigenvectors of Lx in the Lz basis, questioning why one cannot simply solve the secular equation for Lx directly.
  • Another participant clarifies that the matrices provided are already in the Lz basis, implying that finding eigenvectors of Lx will also be done in this basis.
  • A participant raises a hypothetical scenario where Lx, Ly, and Lz are not diagonalized, asking how to find the eigenvectors of Ly in the Lx basis.
  • Some participants suggest that one can find the eigenvalues and eigenvectors for Lx and Ly and then express them in terms of the Lz eigenvectors.
  • There is a discussion about the process of diagonalizing an operator using the eigenvectors of another operator, with questions about the validity of using similarity transformations for this purpose.

Areas of Agreement / Disagreement

Participants generally agree on the process of finding eigenvectors and expressing them in terms of another basis, but there remains some confusion and uncertainty regarding the implications and methods of diagonalization in different bases.

Contextual Notes

Participants express uncertainty about the conditions under which different bases can be used for diagonalization and the assumptions involved in the transformation processes.

KFC
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I am studying QM by myself. I got a quite confusing problem which annoying me for a certain time. Well, this question is about the angular momentum opeator Lx, Ly and Lz. The matrix form for these operatore are given, so by solving the corresponding secular equation, it is easy to find the corresponding eigenvalues and eigenvectors. Here, Lz is given in a diagonalized form, so one can directly obtain the eigenvalues by reading the diagonal elements. Let's say the eigenvalues for Lz is a, b and c. And the corresponding eigenvector are

<br /> \left(<br /> \begin{matrix}<br /> 1 \\ 0 \\ 0<br /> \end{matrix}<br /> \right), \qquad<br /> \left(<br /> \begin{matrix}<br /> 0 \\ 1 \\ 0<br /> \end{matrix}<br /> \right),\qquad<br /> \left(<br /> \begin{matrix}<br /> 0 \\ 0 \\ 1<br /> \end{matrix}<br /> \right)<br />

But I got a question "To find the eigenvectors of Lx in the Lz basis", I have no idea what does it mean? Since we already know the form of Lx operator, what can't we just solve the secular equation to find the eigenvectors? What is the significance of written the eigenvectors of Lx in Lz basis?
 
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KFC said:
I am studying QM by myself. I got a quite confusing problem which annoying me for a certain time. Well, this question is about the angular momentum opeator Lx, Ly and Lz. The matrix form for these operatore are given, so by solving the corresponding secular equation, it is easy to find the corresponding eigenvalues and eigenvectors. Here, Lz is given in a diagonalized form, so one can directly obtain the eigenvalues by reading the diagonal elements. Let's say the eigenvalues for Lz is a, b and c. And the corresponding eigenvector are

<br /> \left(<br /> \begin{matrix}<br /> 1 \\ 0 \\ 0<br /> \end{matrix}<br /> \right), \qquad<br /> \left(<br /> \begin{matrix}<br /> 0 \\ 1 \\ 0<br /> \end{matrix}<br /> \right),\qquad<br /> \left(<br /> \begin{matrix}<br /> 0 \\ 0 \\ 1<br /> \end{matrix}<br /> \right)<br />

But I got a question "To find the eigenvectors of Lx in the Lz basis", I have no idea what does it mean? Since we already know the form of Lx operator, what can't we just solve the secular equation to find the eigenvectors? What is the significance of written the eigenvectors of Lx in Lz basis?

The matrices you are given are already in the Lz basis. Everything you are doing is "in the Lz basis". When you find the eigenvectors of Lx you will be finding those eigenvectors "in the Lz basis".
 
olgranpappy said:
The matrices you are given are already in the Lz basis. Everything you are doing is "in the Lz basis". When you find the eigenvectors of Lx you will be finding those eigenvectors "in the Lz basis".

Why? How do you tell that? Still confusing ...

What about this, if it gives me Lx, Ly and Lz and all of them are not diagonalized matrices. This time, I need to find the eigenvectors of Ly in Lx basis, how can I do that? Sorry, I am not majoring in physics. But I do interest in it so I am learning by myself.
 
Last edited:
You find the eigen-values and eigen-vectors for the L_x and L_y then see how they can be written in terms of the L_z eigen-vectors.
 
Dr Transport said:
You find the eigen-values and eigen-vectors for the L_x and L_y then see how they can be written in terms of the L_z eigen-vectors.

Oh, I got it. That is, we use the usual way to find the eigenvectors and then EXPAND it with those of Lz, is that right?

Thanks
 
KFC said:
Oh, I got it. That is, we use the usual way to find the eigenvectors and then EXPAND it with those of Lz, is that right?

Thanks

Exactly...
 
Equivalently, an operator A is represented by a diagonal matrix in the "A basis".
 
Avodyne said:
Equivalently, an operator A is represented by a diagonal matrix in the "A basis".

So, it means if I solve the secular equation for Lx to find the corresponding eigenvalues and eigenvectors, I actually diagonalize it with a matrix composing of Lx's eigenvectors?

If so, can I use Lz's eigenvectors to form a matrix (says S), and then use the similarity transformation on Lx (with S) to diagonalize Lx? I don't how if this works!?
 

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