Feynman rules for Yukawa theory

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Discussion Overview

The discussion revolves around the derivation of Feynman rules for Yukawa theory, specifically focusing on both scalar and pseudo-scalar cases. Participants also explore the implications of these rules in the context of fermion decay processes.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • One participant requests resources for a complete derivation of Feynman rules for Yukawa theory and examples of fermion decay applications.
  • Another participant mentions that Srednicki's QFT book covers pseudo-scalar Yukawa theory.
  • It is asserted that in the simplest Yukawa theory, fermion number conservation prevents the decay of fermions.
  • A participant discusses the Hamiltonian for the theory, questioning whether the inclusion of the hermitian conjugate affects the decay process.
  • Further clarification is provided regarding the U(1) symmetry of the theory, which leads to the conservation of fermion number and implies that the fermion cannot decay.
  • Participants note that there are no Feynman diagrams that can represent the decay of the fermion in this context.

Areas of Agreement / Disagreement

Participants generally agree on the conservation of fermion number in the simplest Yukawa theory, which prevents fermion decay. However, there is some debate regarding the implications of the Hamiltonian and the role of the hermitian conjugate.

Contextual Notes

The discussion does not resolve the implications of the Hamiltonian on decay processes, nor does it clarify the potential for more complex theories that might allow for fermion decay.

lefebvre
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Hi. Do you know any book/paper/lecture notes where I can find complete derivation of Feynman rules for both scalar and pseudo-scalar Yukawa theory, and maybe an example of application to decay of fermion?
 
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Srednicki's QFT book does pseudoscalar Yukawa theory.

lefebvre said:
maybe an example of application to decay of fermion?

The fermion won't decay in a Yukawa theory because the fermion number is conserved. Unless you have something more than the simplest theory in mind?
 
The_Duck said:
The fermion won't decay in a Yukawa theory because the fermion number is conserved. Unless you have something more than the simplest theory in mind?

OK, I can see that the hamiltonian is: H_{I}=g\phi\bar{\psi}\psi+h.c.
And I have to use it to fermion decay. Isn't this the simplest Yukawa theory? Does this hermitian conjugate make different?
 
lefebvre said:
OK, I can see that the hamiltonian is: H_{I}=g\phi\bar{\psi}\psi+h.c.
And I have to use it to fermion decay. Isn't this the simplest Yukawa theory? Does this hermitian conjugate make different?

Are you talking about decay of the ##\psi## particle? There is a U(1) symmetry ##\psi \to e^{i \theta} \psi## under which the Hamiltonian is invariant. This leads to conservation of ##\psi## number. So the ##\psi## particle can't decay. Said another way, in this theory there are no Feynman diagrams you can draw that represent the decay of a ##\psi## particle.
 

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