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Antineutron
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The antineutron is the of the with symbol . It differs from the neutron only in that some of its properties have . It has the same as the neutron, and no net , but has opposite (+1 for neutron, −1 for the antineutron). This is because the antineutron is composed of , while neutrons are composed of . The antineutron consists of one and two .


Background
The antineutron was discovered in proton–antiproton collisions at the (Lawrence Berkeley National Laboratory) by the team of , Glen Lambertson, , and William Wenzel in 1956, one year after the was discovered.

Since the antineutron is electrically neutral, it cannot easily be observed directly. Instead, the products of its with ordinary matter are observed. In theory, a free antineutron should into an , a , and a in a process analogous to the of . There are theoretical proposals of neutron–antineutron oscillations, a process that implies the violation of the conservation. There is a project to search for neutron-antineutron oscillations using ultracold neutrons.


Magnetic moment
The of the antineutron is the opposite of that of the neutron. It is for the antineutron but for the neutron (relative to the direction of the spin). Here μN is the .


See also
  • Neutron magnetic moment
  • List of particles


External links

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