On-shell renormalization scheme: Difference between revisions

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:<math>Z_2=1+\delta_2</math>
:<math>m?rm_r = m + \delta m</math>
 
On the other hand, the modification to the propagator can be calculated up to a certain order in <math>e</math> using Feynman diagrams. These modifications are summed up in the fermion [[self energy]] <math>\Sigma(p)</math>