- #1
CAF123
Gold Member
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This is probably a simple question but puzzled me a little when trying to explain something to somebody. In all resources online and in most books I've seen, the triple gluon vertex has no overall 'i' factor while e.g. the four gluon vertex always does. The photon and gluon propagators as well as the 3 point quark and gluon/photon vertices also have an 'i'.
Is there a conceptual reason for this?
Looking in Yndurain's book, 'Relativistic QM and intro. to field theory', however, there is an overall 'i' factor in the triple gluon vertex, while the other Feynman rules continue to also have an overall 'i'. This means in some computation, depending on the Feynman rules used, one may get a relative 'i' factor between diagrams contributing to an amplitude (instead of e.g. a relative sign). Of course, an overall 'i' for the amplitude is irrelevant but not a relative 'i' between diagrams.
So, how would one reconcile the two approaches?
Is there a conceptual reason for this?
Looking in Yndurain's book, 'Relativistic QM and intro. to field theory', however, there is an overall 'i' factor in the triple gluon vertex, while the other Feynman rules continue to also have an overall 'i'. This means in some computation, depending on the Feynman rules used, one may get a relative 'i' factor between diagrams contributing to an amplitude (instead of e.g. a relative sign). Of course, an overall 'i' for the amplitude is irrelevant but not a relative 'i' between diagrams.
So, how would one reconcile the two approaches?