Constructing a Feynman loop integral

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Homework Help Overview

The discussion revolves around constructing a Feynman loop integral related to a particle physics diagram involving a left-handed neutrino, a scalar particle, and a heavy Majorana neutrino. Participants are exploring the implications of the Feynman rules and the characteristics of the particles involved.

Discussion Character

  • Exploratory, Conceptual clarification, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to relate the problem to the self-energy of the electron and questions the appropriate Feynman rules for a scalar propagator. They also inquire about the treatment of left-handed neutrinos and the differences in propagators for Dirac versus Majorana particles.

Discussion Status

Some participants suggest that starting from a Lagrangian would provide a clearer path to deriving the necessary Feynman rules, while the original poster expresses uncertainty about transitioning from the Lagrangian to the integral. There is an ongoing exploration of how to properly construct the integral based on the provided information.

Contextual Notes

The original poster mentions being instructed to construct the integral from Feynman rules without further guidance, indicating potential constraints in the information available for the problem.

ryanwilk
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Homework Statement



I need to construct the Feynman loop integral for the following diagram:

loop.jpg
(*)

where \nuL is the left-handed neutrino, \phi is a scalar particle and N is a heavy neutrino with a Majorana mass.

Homework Equations



N/A

The Attempt at a Solution



I'm trying to determine it by comparing it to the self-energy of the electron:

200px-SelfE.svg.png


which gives

self-energy.jpg
.

1) Since there's a scalar propagator (\phi) in (*), do I need to use these Feynman rules?:

yukawa.jpg


where m = m\phi in this case. (Taken from http://bolvan.ph.utexas.edu/~vadim/Classes/2011f/QED.pdf).

2) How do I deal with the fact that the neutrinos are left-handed? Do I just add factors of (1-γ5)/2 in the (-igδβα) terms?

3) For Dirac particles, the propagator is:

dirac.jpg


But how does this change if the particle (in this case, N) is Majorana?Any help would be appreciated.

Thanks!
 
Last edited:
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Have you been given a Lagrangian? It would be much better to work out the Feynman rules from that rather than try to guess at bits and pieces that might not quite fit what you want.
 
The Lagrangian is:

L = L\varphi + LSM where

L\varphi = \frac{1}{2}∂μ\phi+μ\phi + \frac{m^2}{2}\phi+\phi + \frac{λ}{4}(\phi+\phi)2 + g\phi\overline{N_R}\nuL + \frac{m_N}{2}NRTCNR + h.c.

(g = coupling constant, N = Majorana neutrino, \phi = Neutral scalar, \nuL = LH neutrino),

However, I was told just to construct it from Feynman rules. Also, I have no idea how to go from this complicated Lagrangian to the integral =/.
 
Last edited:
Anyone? :frown:
 

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