The loss of quantum coherence in neutrinos due to interactions in dense environments.Neutrino quantum decoherence is the process by which neutrinos lose their quantum mechanical phase relationships when propagating through dense matter, such as the interior of a supernova or the early universe. Neutrinos are produced in definite flavor states (electron, muon, tau) but propagate as superpositions of mass states, leading to oscillations. In dense environments, interactions with background particles can collapse these superpositions, suppressing oscillations and altering the neutrino flux.
The concept of neutrino decoherence in matter was explored in the 1980s and 1990s, with significant theoretical work by Stodolsky and others, but it gained prominence with the study of supernova neutrinos in the 2000s.
When a neutrino scatters off electrons or other neutrinos in a dense medium, the interaction can 'measure' its flavor or energy, effectively collapsing the quantum state. This is analogous to how a measurement destroys interference in a double-slit experiment. In extreme cases, the neutrino ensemble can become fully decoherent, meaning each neutrino is in a definite state, and oscillations cease. However, collective effects—where neutrinos interact with each other—can lead to complex phenomena like synchronized oscillations or even decoherence in a different manner.
Understanding neutrino decoherence is crucial for interpreting signals from supernovae, which could reveal the physics of dense matter and the mechanisms of stellar explosions.
Neutrinos are so weakly interacting that a light-year of lead would block only about half of them, yet in a supernova core, they are so dense that they can decohere within centimeters.
| \tilde{\kappa} | variable | Fourier transform of convergence — convergence |
| \tilde{\kappa}_B | variable | Fourier transform of B-mode convergence — b mode convergence |
| \tilde{\gamma}_1 | variable | Fourier transform of first shear component — shear component |
| \tilde{\gamma}_2 | variable | Fourier transform of second shear component — shear component |
| k_1 | variable | First component of wave vector — wave vector component radian per metre |
| k_2 | variable | Second component of wave vector — wave vector component radian per metre |
| k | variable | Magnitude of wave vector — wave number radian per metre |
| m^* | variable | Effective nucleon mass in the medium — effective mass kilogram |
| m | variable | Bare nucleon mass (in vacuum) — mass kilogram |
| \sigma | variable | Scalar meson field expectation value — scalar field |
| g_\sigma | constant | Coupling constant between nucleons and the scalar sigma meson — coupling constant = varies (model-dependent) |
| f | variable | Gravitational wave frequency — frequency hertz |
| h_0 | variable | Dimensionless Hubble constant (H_0/100 km/s/Mpc) — reduced hubble constant |
| Ω_GW | variable | Gravitational wave energy density per logarithmic frequency — gravitational wave energy density parameter |
| ΔN_eff | variable | Effective number of extra neutrino species — effective neutrino number |
| ∫ d ln f | operator | Integration over logarithmic frequency — logarithmic integral |






