{{Infobox Particle
| bgcolour =
| name = Antineutrino
| image =
| caption =
| num_types = 3 - electron, muon and tau
| composition =
Elementary particle
| family =
Fermion
| group =
Lepton, Anti-Lepton
| generation =
| interaction =
weak force and
gravity
| particle =
| antiparticle =
Neutrino
| theorized = 1930
| discovered = 1956
| symbol =
,
and
| mass =
| decay_time =
| decay_particle =
| electric_charge = 0
| color_charge = 0
| spin = 1/2
| lepton_number = -1
| num_spin_states =
}}
In
physics, 'antineutrinos', the
antiparticles of
neutrinos, are
neutral particles produced in
nuclear beta decay. They have a
spin of 1/2, and they are part of the
lepton family of particles. The antineutrinos observed so far all have right-handed
helicity (i.e., only one of the two possible spin states has ever been seen), while the
neutrinos are left-handed. Antineutrinos interact with other
matter only through the
gravitational and
weak forces, making them very difficult to detect experimentally.
Neutrino oscillation experiments indicate that antineutrinos have
mass, but
beta decay experiments constrain that mass to be very small.
Because antineutrinos and neutrinos are neutral particles it is possible that they are actually the same particle. Particles which have this property are known as
Majorana particles. If neutrinos are indeed Majorana particles then the
neutrinoless double beta decay process is allowed. Several experiments have been proposed to search for this process.
Sandia National Laboratories is researching the use of antineutrino detectors to monitor
nuclear reactors, and to detect very low yield
nuclear tests; such tests with yield under 1
kiloton are difficult to detect using conventional
seismic detectors if evasive methods like eg. seismic decoupling are used.
Spectral analysis of antineutrinos produced by the reactors can be used to remotely assert the isotopic composition of the reactor core.
[1]
See also
★
Neutrino
★
Kamioka Liquid Scintillator Antineutrino Detector
External links
★
Search for neutrinoless double beta decay with enriched 76Ge in Gran Sasso 1990–2003