Antineutron
Subatomic particle
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Related on Lably
Through Neutron, Mass and Electric charge
Background
The antineutron was discovered in proton–antiproton collisions at the Bevatron (Lawrence Berkeley National Laboratory) by the team of Bruce Cork, Glen Lambertson, Oreste Piccioni, and William Wenzel in 1956, one year after the antiproton was discovered.
Since the antineutron is electrically neutral, it cannot easily be observed directly. Instead, the products of its annihilation with ordinary matter are observed. In theory, a free antineutron should decay into an antiproton, a positron, and a neutrino in a process analogous to the beta decay of free neutrons. There are theoretical proposals of neutron–antineutron oscillations, a process that implies the violation of the baryon number conservation. There is a project to search for neutron-antineutron oscillations using ultracold neutrons.
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Magnetic moment
The magnetic moment of the antineutron is the opposite of that of the neutron. It is +1.91 μN for the antineutron but −1.91 μN for the neutron (relative to the direction of the spin). Here μN is the nuclear magneton.

