Pauli Spin Matrices - Lowering Operator - Eigenstates

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Homework Help Overview

The discussion revolves around the Pauli spin matrices, specifically the lowering operator ##\sigma_{-}## and its effect on the eigenstates of the ##\sigma_{z}## operator. The original poster seeks clarification on how the application of ##\sigma_{-}## results in eigenstates of ##\sigma_{z}## and the implications of these results.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the mathematical construction of the lowering operator and its application to the eigenstates of ##\sigma_{z}##. Questions arise regarding the interpretation of the resulting states, particularly the significance of obtaining a zero vector and how it relates to eigenvalues.

Discussion Status

There is an ongoing exploration of the implications of the lowering operator on the eigenstates of ##\sigma_{z}##. Some participants provide insights into the nature of eigenvectors and the expected changes in eigenvalues, while others express confusion about specific results and their physical meaning.

Contextual Notes

Participants note the importance of distinguishing between non-zero eigenstates and the implications of the lowering operator's action, as well as the potential mix-up regarding eigenvalues derived from previous parts of the question.

ChrisJ
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This is not part of my coursework but a question from a past paper (that we don't have solutions to).

1. Homework Statement

Construct the matrix ##\sigma_{-} = \sigma_{x} - i\sigma_{y}## and show that the states resulting from ##\sigma_{-}## acting on the eigenstates of ##\sigma_{z} ## are also eigenstates of ##\sigma_{z} ## and comment on your result.

Homework Equations


pauli spin matrices

The Attempt at a Solution


I need more help with the commenting on the result and the actual physics rather than the maths here,

I constructed the matrix ##\sigma_{-} =
\left( \begin{array}{ccc}
0 & 0 \\
2 & 0 \end{array}
\right)
##

and in previous bit of question found the eigenstates of ##\sigma_{z}## to be ##
\left( \begin{array}{ccc}
1 \\
0 \end{array}\right) ## and ##
\left( \begin{array}{cc}
0 \\
1 \end{array}\right)## respectively.

So therefore ##\sigma_{-}
\left( \begin{array}{ccc}
1 \\
0 \end{array}\right)
=2
\left( \begin{array}{ccc}
0 \\
1 \end{array}\right)##

and also ##\sigma_{-}
\left( \begin{array}{ccc}
0 \\
1 \end{array}\right) =
\left( \begin{array}{ccc}
0 \\
0 \end{array}\right)##

I am pretty sure the math is correct as I ran the math past a few people who agreed but I can't see how/why that that shows they are also eigenstates of ##\sigma_{z}##. I can maybe see it mathematically with the first result, as that is explicitly an eigenstate, but the zero matrix result, I am not sure how in words I can say that it is. And what it means physically. As I said this isn't part of any coursework, just a question from a past exam paper, any help/advice is much appreciated.
 
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An eigenvector is defined to be a non-zero vector, so the statement that the resulting vector is an eigenstate of ##\sigma_z## as mentioned in the question shall only apply to cases when the resulting vector is non-zero.
As for the comment, I think it asks you about how ##\sigma_-## changes the eigenvector of ##\sigma_z##, for example how the eigenvalue changes.
 
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blue_leaf77 said:
An eigenvector is defined to be a non-zero vector, so the statement that the resulting vector is an eigenstate of ##\sigma_z## as mentioned in the question shall only apply to cases when the resulting vector is non-zero.
As for the comment, I think it asks you about how ##\sigma_-## changes the eigenvector of ##\sigma_z##, for example how the eigenvalue changes.
Ah ok, that zero vector/matrix was throwing me. Ok so its just as simple as saying that it lowers the eigenvalue by one? A previous part of the question was to find the eigenvalue of ##\sigma_z## and was found to be 3 and 3.
 
ChrisJ said:
Ah ok, that zero matrix was throwing me. Ok so its just as simple as saying that it lowers the eigenvalue by one? A previous part of the question was to find the eigenvalue of ##\sigma_z## and was found to be 3 and 3.
At least that's the most notable property of ##\sigma_-##.
 
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ChrisJ said:
Ah ok, that zero vector/matrix was throwing me. Ok so its just as simple as saying that it lowers the eigenvalue by one? A previous part of the question was to find the eigenvalue of ##\sigma_z## and was found to be 3 and 3.
3 and 3?
 
vela said:
3 and 3?

Sorry, worded that wrong. Meant to say that I found the eigenvalues of the two eigenstates to be 3 and 3.
 
That's what I thought you meant, but you should have found them to be 1 and -1.
 
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ChrisJ said:
was found to be 3 and 3.
Not sure why I missed that, but that's clearly not true.
 
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vela said:
That's what I thought you meant, but you should have found them to be 1 and -1.
blue_leaf77 said:
Not sure why I missed that, but that's clearly not true.

My bad! I did the previous bit of the question a couple weeks ago, sorry my fault. It seems the 3 and 3 I had in my head was not about that, it was to find the eigenvalues of ##\sigma^2=\sigma_x^2+\sigma_y^2+\sigma_z^2 ## Sorry for the confusion. I just remembered in my head that I found eigenvalues and they were 3, so when I went back to do the rest of the multiple part question, I had those 3's in my head.
 
  • #10
But now that you pointed out the mix up. My original question about commenting on the result ##\sigma_{-}## acting on ##\sigma_z##? as when the lowering operator acts on ##\sigma_z## it results in an eigenstate of ##\sigma_z## but with an eigenvalue of 2, but its original eigenvalues were 1 and -1?
 
  • #11
ChrisJ said:
But now that you pointed out the mix up. My original question about commenting on the result ##\sigma_{-}## acting on ##\sigma_z##? as when the lowering operator acts on ##\sigma_z## it results in an eigenstate of ##\sigma_z## but with an eigenvalue of 2, but its original eigenvalues were 1 and -1?
No, the constant 2 in ##\sigma_- |+\rangle = 2 |-\rangle## is not the eigenvalue - it should be obvious that this equation is not an eigenvalue equation. What ##\sigma_-## does is that it changes the eigenstate of ##\sigma_z## to another eigenstate whose eigenvalue is one unit smaller than that of the initial eigenstate. Lowering operator, for more general angular momentum operator, obeys the condition ##L_z L_- |n\rangle = (n-1)\hbar L_- |n\rangle## where ##|n\rangle## is an eigenstate of ##L_z##.
 
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