Pauli Spin Matrices - Lowering Operator - Eigenstates

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SUMMARY

The discussion focuses on the Pauli lowering operator, represented as ##\sigma_{-} = \sigma_{x} - i\sigma_{y}##, and its effect on the eigenstates of the Pauli spin matrix ##\sigma_{z}##. The participants confirm that applying ##\sigma_{-}## to the eigenstates of ##\sigma_{z}## results in new eigenstates, with the eigenvalue decreasing by one unit. The eigenstates of ##\sigma_{z}## are identified as ##\left( \begin{array}{ccc} 1 \\ 0 \end{array}\right)## and ##\left( \begin{array}{ccc} 0 \\ 1 \end{array}\right)##, leading to a clear understanding that the zero vector indicates a transition to a non-existent state, reinforcing the concept of eigenvalues in quantum mechanics.

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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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