Antineutrino



Antineutrino
Composition: Neutrino
Theorized: 1930
Discovered: 1956
Symbol: \overline{\nu}_e, \overline{\nu}_\mu and \overline{\nu}_\tau
No. of types: 3 - electron, muon and tau
Electric charge: 0
Color charge: 0
Spin: 1/2

In physics, antineutrinos, the antiparticles of 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 such as 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



Antimatter
Overview
Annihilation
Devices
Antiparticles
Uses
  • PET
  • Fuel
  • Weaponry
Bodies
  • ALPHA Collaboration
  • ATHENA
  • ATRAP
  • CERN
People
  • Paul Dirac
  • Carl D. Anderson
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This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article "Antineutrino". A list of authors is available in Wikipedia.