Subatomic particle
Theantineutron is theantiparticle of theneutron with symboln . It differs from the neutron only in that some of its properties haveequal magnitude but opposite sign . It has the samemass as the neutron, and no netelectric charge , but has oppositebaryon number (+1 for neutron, −1 for the antineutron). This is because the antineutron is composed ofantiquarks , while neutrons are composed ofquarks . The antineutron consists of oneup antiquark and twodown antiquarks .
The antineutron was discovered inproton–antiproton collisions at theBevatron (Lawrence Berkeley National Laboratory ) by the team ofBruce Cork , Glen Lambertson,Oreste Piccioni , and William Wenzel in 1956,[ 2] one year after theantiproton was discovered.
Since the antineutron is electrically neutral, it cannot easily be observed directly. Instead, the products of itsannihilation with ordinary matter are observed. In theory, a free antineutron shoulddecay into anantiproton , apositron , and aneutrino in a process analogous to thebeta decay offree neutrons . There are theoretical proposals ofneutron–antineutron oscillations , a process that implies the violation of thebaryon number conservation.[ 3] [ 4] [ 5] There is a project to search for neutron-antineutron oscillations using ultracold neutrons.[ 6] [ 7] [ 8] [ 9]
Themagnetic moment of the antineutron is the opposite ofthat of the neutron .[ 10] It is +1.91 μ N for the antineutron but −1.91 μ N for the neutron (relative to the direction of thespin ). Hereμ N is thenuclear magneton .
^ "2022 CODATA Value: neutron mass energy equivalent in MeV" .The NIST Reference on Constants, Units, and Uncertainty .NIST . May 2024. Retrieved2024-05-18 .^ Cork, Bruce; Lambertson, Glen R.; Piccioni, Oreste; Wenzel, William A. (15 November 1956)."Antineutrons Produced from Antiprotons in Charge-Exchange Collisions" .Physical Review .104 (4):1193– 1197.Bibcode :1956PhRv..104.1193C .doi :10.1103/PhysRev.104.1193 .S2CID 123156830 . ^ R. N. Mohapatra (2009). "Neutron-Anti-Neutron Oscillation: Theory and Phenomenology".Journal of Physics G .36 (10) 104006.arXiv :0902.0834 .Bibcode :2009JPhG...36j4006M .doi :10.1088/0954-3899/36/10/104006 .S2CID 15126201 . ^ C. Giunti; M. Laveder (19 August 2010)."Neutron Oscillations" .Neutrino Unbound .Istituto Nazionale di Fisica Nucleare . Archived fromthe original on 27 September 2011. Retrieved19 August 2010 . ^ Y. A. Kamyshkov (16 January 2002)."Neutron → Antineutron Oscillations" (PDF) .NNN 2002 Workshop on "Large Detectors for Proton Decay, Supernovae and Atmospheric Neutrinos and Low Energy Neutrinos from High Intensity Beams" at CERN . Archived fromthe original (PDF) on 13 June 2019. Retrieved19 August 2010 . ^ Serebrov, A.; Fomin, A.; Kamyshkov, Y. (2016). "Sensitivity of Experiment on Search for Neutron–Antineutron Oscillations on the Projected Ultracold Neutron Source at the WWR-M Reactor".Technical Physics Letters .42 (1):99– 101.Bibcode :2016TePhL..42...99S .doi :10.1134/S1063785016010314 . ^ A.K. Fomin; et al. (2017)."Experiment on search for neutron–antineutron oscillations using a projected UCN source at the WWR-M reactor" .Journal of Physics: Conference Series .798 (1) 012115.Bibcode :2017JPhCS.798a2115F .doi :10.1088/1742-6596/798/1/012115 . ^ A.K. Fomin (2017)."Experiment On Search For n-nbar Oscillations Using A Projected UCN Source At The WWR-M Reactor" .Proceedings of Science .281 : 189.doi :10.22323/1.281.0189 . ^ A.K. Fomin; et al. (2019)."Project on searching for neutron-antineutron oscillation at the WWR-M reactor" .Journal of Physics: Conference Series .1390 (1) 012133.Bibcode :2019JPhCS1390a2133F .doi :10.1088/1742-6596/1390/1/012133 . ^ Lorenzon, Wolfgang (6 April 2007)."Physics 390: Homework set #7 Solutions" (PDF) .Modern Physics, Physics 390, Winter 2007 . Retrieved22 December 2009 .