I'm studying quantum field theory and I encountered some problems of diffusion of particles by an external potential. Until now I have to do with diffusion of the type particle-particle obtaining the Feynman rules from the Lagrangian of the theory and I don't know how to implement the presence of an external potential. How can I implement it?
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Diffusion means scattering, I guess. The diagram technique exists for external fields too. In QED you write $L_{int} \propto j\cdot A + j\cdot A_{ext}$ and denote $A_{ext}$ as a different from photon line. $A_{ext}$ is a know function of space-time arguments. I saw the corresponding diagrams in many textbooks. You just have to look, for example, at scattering an electron from a nucleus in QED. |
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