Solve Exercise 2.4 in Supergravity by Freedman & Van Proeyen

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The discussion focuses on Exercise 2.4 from the textbook "Supergravity" by Freedman and Van Proeyen, which involves proving the identities involving sigma matrices and SL(2,C) transformations. The identities in question are ## A\bar{\sigma}_\mu A^\dagger=\bar{\sigma}_\nu \Lambda^{-1}{}^\nu{}_\mu## and ##A^\dagger \sigma A=\sigma_\nu \Lambda^\nu{}_\mu##. The user identifies a potential confusion regarding the differences between barred and unbarred sigma matrices, particularly noting that ##\sigma_0 = -1## and ##\bar \sigma_0 = 1##. The user concludes that the identities may hold due to the differing index structures of the sigma matrices.

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Korybut
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Hi there!

I am reading textbook "Supergravity" by Freedman and Van Proeyen and got stuck on a simple exercise (Ex 2.4). Usually I would proceed further marking it as a typo but I've checked the errata list on the website and didn't find this exercise there

Exercise 2.4 Show that ## A\bar{\sigma}_\mu A^\dagger=\bar{\sigma}_\nu \Lambda^{-1}{}^\nu{}_\mu## and ##A^\dagger \sigma A=\sigma_\nu \Lambda^\nu{}_\mu## . This gives precise meaning to the statement that the matrices ##\bar{\sigma}_\mu## and ##\sigma_\nu## are 4-vectors

Sigma matrices in this book are defined as

$$\sigma_\mu=\left(-\mathbb{1},\sigma_i\right),\;\;\; \bar{\sigma}_\mu=\sigma^\mu=\left(\mathbb{1},\sigma_i\right).$$

And SL(2,C) transformations is defined as
$$ \mathbf{x}^\prime \equiv A \mathbf{x} A^\dagger$$

The first identity in the exercise is kinda straightforward and it is also easy to see that the second one holds for barred sigma-matrices. But I didn't managed to work out the identity in the form written in the exercise

Is it a typo or I missing something very deep?
 
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It looks like the only difference between the barred and unbarred sigma matrices is that ##\sigma_0 = -1## while ##\bar \sigma_0 = 1##. Since 1 is just the identity matrix, I don't see how you could have gotten different results for the barred vs. unbarred case.
 
Since it is involved in the contraction on r.h.s. of the identity it makes difference.

This identity is true
$$ A^\dagger \bar{\sigma}_\mu A=\bar{\sigma}_\nu\Lambda^\nu{}_\mu.$$
And it is kinda obvious. When I apply inverse SL(2,C) transformation it should result in inverse Lorentz transformation.

Also one may show the following

$$A^\dagger \sigma_\nu A=\sum_\mu \sigma_\mu \Lambda_\mu{}^\nu$$
(I know that it looks weird from tensor calculus perspective. By writing this I mean one should extract exact values (for particular ##\mu## and ##\nu##)in some referrence frame)

The initial identity is proven if ## \Lambda_\mu{}^\nu=\Lambda^\mu{}_\nu##, but it is not true
 
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After some thinking and asking I believe that this identity may be true due different index structure of sigma matrices

$$ \sigma_{\mu \alpha \dot{\alpha}}, \bar{\sigma}_\mu {}^{\dot{\alpha} \alpha}$$

If someone has a nice comprehensive refference on this spinor algebra issues I would be very thankful.

P.S. It can really drive someone insane when one sees the expression like ## (M^T)_\alpha {}^\beta## without any explanation on the meaning of this notation.
 

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