Invariance of the determinant under spin rotations

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Homework Help Overview

The discussion revolves around demonstrating the invariance of the determinant of a specific 2x2 matrix formed by the dot product of Pauli matrices and a vector. The original poster seeks to understand how to approach this problem involving spin rotations and matrix properties.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss various methods for tackling the problem, including matrix multiplication and the use of commutation relations for Pauli matrices. Some express confusion about the complexity of the calculations and seek alternative approaches or hints.

Discussion Status

The conversation includes attempts to simplify the problem using properties of determinants and Pauli matrices. Some participants have begun to clarify their understanding of the determinant properties, while others are still grappling with specific expressions and calculations. There is an ongoing exploration of different interpretations and methods without a clear consensus.

Contextual Notes

Participants note the challenge of expressing certain terms in a manageable form and the implications of assumptions regarding the determinants of exponential matrices. There is a recognition of the need for clarity on the properties of determinants in relation to the problem at hand.

ShayanJ
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Homework Statement


Show that the determinant of a ##2 \times 2 ## matrix ## \vec\sigma \cdot \vec a ## is invariant under ## \vec \sigma\cdot \vec a \rightarrow \vec \sigma\cdot \vec a' \equiv \exp(\frac{i\vec \sigma \cdot \hat n \phi}{2})\vec \sigma\cdot \vec a \exp(\frac{-i\vec \sigma \cdot \hat n \phi}{2}) ##.

Homework Equations


## \sigma_1=\left( \begin{array}{cc} 0 \ \ \ \ \ \ \ \ 1 \\ 1 \ \ \ \ \ \ \ \ 0 \end{array} \right) ##
## \sigma_2=\left( \begin{array}{cc} 0 \ \ \ \ -i \\ i \ \ \ \ \ \ 0 \end{array} \right) ##
## \sigma_3=\left( \begin{array}{cc} 1 \ \ \ \ \ \ \ \ 0 \\ 0 \ \ \ \ -1 \end{array} \right) ##

##\exp(\frac{\pm i\vec \sigma \cdot \hat n \phi}{2})=\cos{(\frac \phi 2)}\pm i(\vec\sigma \cdot \hat n)\sin{(\frac \phi 2)} ##

The Attempt at a Solution



I tried to do it by matrix multiplication but the calculations turned out to be so much tedious that I thought there should be a better way. If this is the only way, just tell me. Otherwise just point to the right direction. Any other hint is welcome too.
Thanks
 
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You should be able to use the commutation relation for the Pauli matrices ##[\sigma_i , \sigma_j ] = 2 i \epsilon_{ijk} \sigma_k## (sum over ##k## assumed) rather than actually write out explicit matrix products.
 
I used the properties of Pauli matrices and got the following:

## \cos^2 \frac \phi 2 \ (\vec \sigma \cdot \vec a)-i\sin \phi \left[(\vec a \times \hat n)\cdot \vec \sigma \right]+\sin^2\frac \phi 2 \left[(\vec \sigma \cdot \hat n)(\vec a \cdot \hat n )+i \vec a \cdot \vec \sigma- i(\hat n \cdot \vec \sigma)(\vec a \cdot \hat n)\right] ##

But I don't know how to proceed!
 
Shyan said:
I used the properties of Pauli matrices and got the following:

## \cos^2 \frac \phi 2 \ (\vec \sigma \cdot \vec a)-i\sin \phi \left[(\vec a \times \hat n)\cdot \vec \sigma \right]+\sin^2\frac \phi 2 \left[(\vec \sigma \cdot \hat n)(\vec a \cdot \hat n )+i \vec a \cdot \vec \sigma- i(\hat n \cdot \vec \sigma)(\vec a \cdot \hat n)\right] ##

But I don't know how to proceed!

I think that in the ##\sin^2(\phi/2)## term, the 1st and 3rd terms should have the same coefficient (to give an overall ##2(\hat n \cdot \vec \sigma)(\vec a \cdot \hat n)##) and there shouldn't be an ##i## in the 2nd term. If you want to recheck the term, the identity ##\sigma_i \sigma_j = \delta_{ij} I + i \epsilon_ijk}\sigma_k## should be useful (though you might already be aware of it).

So you will have an expression ##\vec{A} \cdot \vec{\sigma}## and you should show that ##\det ( \vec{A} \cdot \vec{\sigma}) = - \vec{A}\cdot \vec{A}##, by explicit muliplication or otherwise. Then apply this to your particular expression.
 
I corrected some mistakes and I got ## \vec A \cdot \vec \sigma ## where ## \vec A=\cos^2 \frac \phi 2 \vec a +\sin \phi (\vec a \times \hat n)+\sin^2 \frac \phi 2 \left[2(\vec a \cdot \hat n)\hat n-\vec a \right] ##.
Now my problem is, ##\vec A \cdot \vec A ## is not a straightforward expression and I can't write it as a function of only ##\vec a \cdot \vec a ##.
 
Can't you just use general properties of determinants?
I.e., ##\det(AB) = \det A \; \det B## and ##\det A^{-1} = 1/\det A##, etc ?

Am I missing something here??
 
thanks strangerep. The determinants of those exponentials are 1 and so things are very simple.
I have this bad habit of always trying the hardest way first!
 
Shyan said:
The determinants of those exponentials are 1 [...]
Actually, you don't even need to know their value... :oldwink:
 
strangerep said:
Actually, you don't even need to know their value... :oldwink:
I don't understand!
 
  • #10
Well, I already noted these properties of determinants:
##\det(AB) = \det A \; \det B## and ##\det\left(A^{-1}\right) = 1/\det A##, so...
$$ \det\left(ABA^{-1}\right) ~=~ ... ~?$$

[Edit: you answered my post before I'd finished. Work out the above...]
 
  • #11
strangerep said:
Well, I already noted these properties of determinants:
##\det(AB) = \det A \; \det B## and ##\det\left(A^{-1}\right) = 1/\det A##,
Yes, but those are useful in proving the invariance only when you know that the determinant of those exponentials are one. But you said I don't need to know the value of the determinants. This is what I don't understand.
 
  • #12
Re-read my post #10...
 

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