QED says, well, thanks to quantum or Feynman and Schwinger, they are exchanging virtual particles.
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And that's the Feynman diagram.
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And what you do is each time you write a Feynman diagram, each one of those lines in the Feynman
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But the virtual particles typically refer to internal lines in the Feynman diagrams.
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No, I'm just trying to figure out, like, how would you draw the Feynman diagram for just a point charge and its field?
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So, you could imagine exactly as you're saying, you know, it's a four-point tree-level scattering Feynman diagram where you have two electrons going in, two electrons going out.
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So, when you do that Feynman diagram and you're integrating over the momentum, you get this delta function from momentum conservation.
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When you write down the Feynman diagrams, you can have what they call tree-level diagrams and then loop-level diagrams.
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you have that Feynman vertex where you have an electron, positron and a photon, there's like
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