Problem about scattering amptitude

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SUMMARY

The discussion focuses on the scattering amplitude of photons and electrons, specifically addressing the averaging of initial and final polarizations in the context of unpolarized photons. The amplitude is represented as f(ϵα(k), ϵα′(k′)), and the process involves averaging over initial polarization and summing over final polarization states. This method is identified as a "partial wave expansion," which simplifies the calculation of the total scattering amplitude by breaking it down into components corresponding to specific angular momentum states.

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Take the scattering of photon and electron as example, we first figure out the amptitude for transition definte polarization,
say f(ϵα(k),ϵα′(k′))
If the initial photon is unpolarized and the final polarization is not observed, we need to average the initial polarization and sum over the possible final polarization.
But why we just average and sum over the two independent polarization,1/2∑α∑α′f? the initial and final polarization should be all possible combination of the independent polarizatition.
 
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How to understand the average and sum?The average and sum over the two independent polarizations is actually what's known as a "partial wave expansion", which is a way of expanding the scattering amplitude into a sum of terms that each correspond to a particular angular momentum. The idea is that the total scattering amplitude can be expressed as a sum of these individual terms, and each term is determined by the initial and final polarizations. By averaging and summing over the two independent polarizations, we are essentially separating out the amplitude into individual components that each correspond to a particular angular momentum. This then allows us to calculate the total scattering amplitude more efficiently.
 

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