
Neutrino decay is the process where neutrinos transform into other particles, reconciling cosmological and laboratory data.Neutrino decay refers to the hypothetical process where a heavier neutrino (e.g., muon or tau neutrino) transforms into a lighter one plus other particles, such as photons or lighter neutrinos. In the Standard Model, neutrinos are stable, but extensions that allow decay could explain discrepancies between cosmological observations (which imply a certain neutrino mass sum) and laboratory measurements (which set tighter bounds). If neutrinos decay, their relic abundance and energy distribution in the early universe would change, potentially resolving the 'missing' neutrino mass problem and affecting structure formation.
The idea of neutrino decay dates back to the 1980s, but gained traction in the 2010s when cosmological data from Planck and baryon acoustic oscillations suggested a neutrino mass sum higher than laboratory limits. Recent analyses (2023–2024) have proposed decay as a reconciliation, though no direct evidence exists.
Neutrino decay requires physics beyond the Standard Model, typically via new interactions or Majorana mass terms. In a simple model, a heavy neutrino decays into a lighter neutrino and a massless or very light boson (e.g., a majoron). The decay rate depends on the coupling strength and mass difference. In cosmology, decaying neutrinos would produce a diffuse background of lighter neutrinos and possibly photons, altering the cosmic microwave background and large-scale structure.
Neutrino decay models are used in cosmology to interpret data from surveys like DESI and Planck, and in particle physics to guide searches for new particles at colliders and neutrino experiments.
If neutrinos decay, they would do so extremely slowly—with lifetimes longer than the age of the universe—but even a tiny decay rate could have shaped the cosmos.
| F | variable | value of the decaying quantity at position x — amplitude varies |
| F_0 | variable | initial value at x = 0 — amplitude varies |
| x | variable | independent variable (position, time, etc.) — position metre |
| α | variable | decay constant (rate of decay per unit x) — decay constant per metre |









