Decompose SL(2C) Matrix: Real Parameters from Complex

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TL;DR
How can an SL(2,C) matrix be decomposed into a product of a boost along the z-axis and a pure rotation?
Hi,

suppose I am given an SL(2C) matrix of the form ##\exp(i\alpha/2 \vec{t}\cdot\vec{\sigma})## where ##\alpha## is the complex rotation angle, ##\vec{t}## the complex rotation axis and ##\vec{\sigma}## the vector of the three Pauli matrices.
I would like to decompose this vector into ##\exp(i\beta/2 \vec{q}\cdot\vec{\sigma})\exp(\gamma\sigma_z)##, where now the rotation angle ##\beta##, axis ##\vec{q}## and the boost parameter ##\gamma## are all real.
Is there a non-brain damaged way to do this? This isn't homework related.

Thank you!
 
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Just a thought, and maybe a silly one as I think in terms of algebra and less in terms of physics.
##\vec{t}\cdot\vec{\sigma}## is a complex number, hence ##\exp(i\alpha/2 \vec{t}\cdot\vec{\sigma})## is of the form ##e^{x+iy}=e^x\cdot e^{iy}##. In case ##\vec{t}\cdot\vec{\sigma}## is real, which I assume, then ##\beta =2\alpha /(\vec{t}\cdot\vec{\sigma}), \gamma =0## and ##\vec{q}## any vector such that ##\vec{q}\cdot\vec{\sigma}=1.##
 
Hi fresh, thank you. No, t sigma is not real. I now saw that my initial assumption is incorrect. You can't decompose a general Lorentz transformation into a boost along the z axis and a rotation. However, you can decompose it into a boost (along a direction which has to be determined) and a rotation. This is in principle a polar decomposition. I found some information in be book by Sexl and Urbantke.
 
I'm not sure, but couldn't one write down the series of the matrix exponential and somehow sort out the real and imaginary parts?
 
DrDu said:
Hi fresh, thank you. No, t sigma is not real. I now saw that my initial assumption is incorrect. You can't decompose a general Lorentz transformation into a boost along the z axis and a rotation. However, you can decompose it into a boost (along a direction which has to be determined) and a rotation. This is in principle a polar decomposition. I found some information in be book by Sexl and Urbantke.
This all sounds like the decomposition of a matrix into its toral (diagonalizable) and nilpotent (upper triangular) part. Within Lie algebras it is called Malcev decomposition or Jordan-Chevalley. I asssume the latter holds for groups, too.
 
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Of course, but this wouldn't provide much insight.
fresh_42 said:
This all sounds like the decomposition of a matrix into its toral (diagonalizable) and nilpotent (upper triangular) part. Within Lie algebras it is called Malcev decomposition or Jordan-Chevalley. I asssume the latter holds for groups, too.
Yes, it is similar. In this case it is the polar decomposition, i.e. the decomposition of a normal matrix into the product of a hermitian and a unitary one.
 
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