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The antineutron is the antiparticle of the neutron with symbol n. It differs from the neutron only in that some of its properties have equal magnitude but opposite sign.It has the same mass as the neutron, and no net electric charge, but has opposite baryon number (+1 for neutron, −1 for the antineutron).
The neutrino [a] was postulated first by Wolfgang Pauli in 1930 to explain how beta decay could conserve energy, momentum, and angular momentum ().In contrast to Niels Bohr, who proposed a statistical version of the conservation laws to explain the observed continuous energy spectra in beta decay, Pauli hypothesized an undetected particle that he called a "neutron", using the same -on ending ...
==Summary== {{en|The Feynman Diagram for the beta negative decay of a neutron into a proton. The down quark in the neutron decays into an up quark to make a proton, emitting an electron and an electron anti-neutrino.}} ==Source== Created by [[User:Joelhol: 09:13, 9 March 2007: 310 × 310 (22 KB) Joelholdsworth~commonswiki
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The electron neutrino has a corresponding antiparticle, the electron antineutrino (ν e), which differs only in that some of its properties have equal magnitude but opposite sign. One major open question in particle physics is whether neutrinos and anti-neutrinos are the same particle.
The two types of beta decay are known as beta minus and beta plus.In beta minus (β −) decay, a neutron is converted to a proton, and the process creates an electron and an electron antineutrino; while in beta plus (β +) decay, a proton is converted to a neutron and the process creates a positron and an electron neutrino. β + decay is also known as positron emission.
The Feynman diagram for beta-minus decay of a neutron (n = udd) into a proton (p = udu), electron (e −), and electron anti-neutrino ν e, via a charged vector boson (W −). In one type of charged current interaction, a charged lepton (such as an electron or a muon, having a charge of −1) can absorb a W +
The left-handed anti-neutrino has a B − L of +1 and an X charge of +5. Due to the lack of electric charge, hypercharge, and color charge, sterile neutrinos would not interact via the electromagnetic, weak, or strong interactions, making them extremely difficult to detect.