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Beta particles
Beta particles







As in all nuclear decays, the decaying element (in this case 14 This new element has an unchanged mass number A, but an atomic number Z that is increased by one. In this form of decay, the original element becomes a new chemical element in a process known as nuclear transmutation. Since a proton or neutron has lepton number zero, β + decay (a positron, or antielectron) must be accompanied with an electron neutrino, while β − decay (an electron) must be accompanied by an electron antineutrino.Īn example of electron emission (β − decay) is the decay of carbon-14 into nitrogen-14 with a half-life of about 5,730 years: These particles have lepton number +1, while their antiparticles have lepton number −1. īeta decay conserves a quantum number known as the lepton number, or the number of electrons and their associated neutrinos (other leptons are the muon and tau particles). β + decay is also known as positron emission.

#Beta particles 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. The two types of beta decay are known as beta minus and beta plus.

beta particles

  • 10 Helicity (polarization) of neutrinos, electrons and positrons emitted in beta decay.
  • 6.2 Stability of naturally occurring nuclides.
  • 2.1 Discovery and initial characterization.
  • In electron capture, an inner atomic electron is captured by a proton in the nucleus, transforming it into a neutron, and an electron neutrino is released. For example, a neutron, composed of two down quarks and an up quark, decays to a proton composed of a down quark and two up quarks.Įlectron capture is sometimes included as a type of beta decay, because the basic nuclear process, mediated by the weak force, is the same. Nucleons are composed of up quarks and down quarks, and the weak force allows a quark to change its flavour by emission of a W boson leading to creation of an electron/antineutrino or positron/neutrino pair. For either electron or positron emission to be energetically possible, the energy release ( see below) or Q value must be positive.īeta decay is a consequence of the weak force, which is characterized by relatively lengthy decay times. The binding energies of all existing nuclides form what is called the nuclear band or valley of stability. The probability of a nuclide decaying due to beta and other forms of decay is determined by its nuclear binding energy. By this process, unstable atoms obtain a more stable ratio of protons to neutrons.

    beta particles

    Neither the beta particle nor its associated (anti-)neutrino exist within the nucleus prior to beta decay, but are created in the decay process. For example, beta decay of a neutron transforms it into a proton by the emission of an electron accompanied by an antineutrino or, conversely a proton is converted into a neutron by the emission of a positron with a neutrino in so-called positron emission.

    beta particles

    In nuclear physics, beta decay (β-decay) is a type of radioactive decay in which a beta particle (fast energetic electron or positron) is emitted from an atomic nucleus, transforming the original nuclide to an isobar of that nuclide.







    Beta particles