Z-Boson Decays into Majorana or Dirac (Heavy) Neutrinos
arXiv:2105.06576 · doi:10.1103/PhysRevD.104.055027
Abstract
We computed the kinematics of Z-boson decay into a heavy-light neutrino pair when the Z-boson is produced at rest in electron-positron collisions, including the subsequent decay of the heavy neutrino into a visible final state containing a charged-lepton. We concentrated on heavy-neutrino masses of order dozens of GeV and the issue of addressing the nature of the neutrinos - Dirac fermions or Majorana fermions. We find that while it is not possible to tell the nature of the heavy and light neutrinos on an event-by-event basis, the nature of the neutrinos can nonetheless be inferred given a large-enough sample of heavy-light neutrino pairs. We identify two observables sensitive to the nature of neutrinos. One is the forward-backward asymmetry of the daughter-charged-leptons. This asymmetry is exactly zero if the neutrinos are Majorana fermions and is non-zero (and opposite) for positively- and negatively-charged daughter-leptons if the neutrinos are Dirac fermions. The other observable is the polarization of the heavy neutrino, imprinted in the laboratory-frame energy distribution of the daughter-charged-leptons. Dirac neutrinos and antineutrinos produced in electron-positron collisions at the Z-pole are strongly polarized while Majorana neutrinos are at most as polarized as the -bosons.
12 pages, 7 figures, references added in v2, results and conclusions unchanged
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- Monojet search for heavy neutrinos at future -factories
- New Physics Search at the CEPC: a General Perspective
- New Particles at the Z-Pole: Tera-Z factories as discovery and precision machines
- Constraints on Heavy Neutral Leptons interacting with a singlet scalar
- Characterizing Heavy Neutral Fermions via their Decays