Dirac Vs. Majorana Neutrino Masses From a TeV Interval

TL;DR

This paper explores whether neutrinos are Dirac or Majorana particles within a five-dimensional supersymmetric model, showing that boundary conditions and localization effects determine their nature and mass scale.

Contribution

It demonstrates how boundary configurations and localization in a 5D model influence neutrino mass types and sizes, providing conditions for Dirac or Majorana neutrinos.

Findings

Majorana masses generally arise for neutrinos with generic boundary terms.

Specific boundary conditions can lead to Dirac neutrinos due to conserved lepton number.

Neutrino masses in the sub-eV range require particular localization or coupling parameters.

Abstract

We investigate the nature (Dirac vs. Majorana) and size of left-handed neutrino masses in a supersymmetric five-dimensional model compactified in the interval [0,\pi R], where quarks and leptons are localized on the boundaries while the gauge and Higgs sectors propagate in the bulk of the fifth dimension. Supersymmetry is broken by Scherk-Schwarz boundary conditions and electroweak breaking proceeds through radiative corrections. Right-handed neutrinos propagate in the bulk and have a general five-dimensional mass M, which localizes the zero modes towards one of the boundaries, and arbitrary boundary terms. We have found that for generic boundary terms left-handed neutrinos have Majorana masses. However for specific boundary configurations left-handed neutrinos are Dirac fermions as the theory possesses a conserved global U(1) symmetry which prevents violation of lepton number. The size of neutrino masses depends on the localization of the zero-modes of right-handed neutrinos and/or the size of the five-dimensional neutrino Yukawa couplings. Left-handed neutrinos in the sub-eV range require either MR~10 or Yukawa couplings ~10^{-3}R, which make the five-dimensional theory perturbative up to its natural cutoff.