Difference between revisions of "Differential Cross-Section"
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<center><math>\cos{\theta}=-1+\cos{\frac{\theta}{2}}</math></center> | <center><math>\cos{\theta}=-1+\cos{\frac{\theta}{2}}</math></center> | ||
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+ | In the ultra-relativistic limit, the electron mass is small enough compared to the energy such that it can be neglected when compared to the momentum | ||
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+ | <center><math>E^2\equiv m^2+p^2 \approx E^2=p^2</math></center> | ||
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Revision as of 14:21, 29 June 2017
Differential Cross-Section
Using the fine structure constant
In the center of mass frame the Mandelstam variables are given by:
Using the relationship
In the ultra-relativistic limit, the electron mass is small enough compared to the energy such that it can be neglected when compared to the momentum