Invariance of the determinant under spin rotations

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SUMMARY

The determinant of a 2x2 matrix represented as ##\vec\sigma \cdot \vec a## is invariant under spin rotations defined by the transformation ##\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})##. The properties of the Pauli matrices, specifically the commutation relation ##[\sigma_i , \sigma_j ] = 2 i \epsilon_{ijk} \sigma_k##, are essential for simplifying the calculations. The determinant of the exponentials involved in the transformation is 1, which simplifies the proof of invariance. The final expression for the transformed matrix can be derived using these properties without explicit matrix multiplication.

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  • Understanding of 2x2 matrices and determinants
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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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