Let's assume seesaw 1 type of generation of left neutrino Majorana mass:
Lm=−Gij(ˉνLˉlL)iiσ2(φ∗1φ∗2)νjR−Mij(νTR)iˆCνjR+h.c.
After using the unitary gauge and shifting the vacuum we can get the mass terms
Lm=−12(νLνcR)TˆC−1(0ˆm∗Dˆm†DˆM†)(νLνcR)+h.c.,
where
νc=ˆCˉνT,ˆmijD=ηGij,
and interaction terms with the Higgs field σ:
Lint=−σGijˉνiLνjR+h.c.
We can "diagonalize"
(1) if we assume that
||mD||<<||M||:
Lm≈νTLˆM1νL−νTRˆM2νR+h.c.,ˆM1=−ˆmTDˆM−1ˆmD,ˆM2=ˆM.
But how to "delete" interaction term
(2) (i.e., to integrate out heavy field
νR)?
This post imported from StackExchange Physics at 2014-08-09 08:47 (UCT), posted by SE-user Andrew McAddams