The discussion centers on the derivation of Feynman rules for scalar and pseudo-scalar Yukawa theory, with a specific interest in applications related to fermion decay. It is clarified that in the simplest Yukawa theory, fermion number conservation prevents the decay of fermions, as indicated by the U(1) symmetry of the Hamiltonian. The Hamiltonian presented, H_{I}=g\phi\bar{\psi}\psi+h.c., does not allow for decay processes involving the fermion particle. Participants emphasize that no Feynman diagrams can represent the decay of the fermion in this theoretical framework. Overall, the conservation laws in Yukawa theory restrict fermion decay despite the presence of interaction terms.