Beta plus and beta minus decay
Beta plus and beta minus decay require a change in quark character. Repeating the equation for beta minus decay:
The weak interaction converts a neutron into a proton while emitting an electron and an anti-neutrino. At the fundamental level (as depicted in the Feynman diagram below), this is due to the conversion of a down quark to an up quark by emission of a W− boson; the W− boson subsequently decays into an electron and an anti-neutrino.
An example of beta minus emission is carbon 14 decay into nitrogen:
Beta plus decay
In beta plus decay
Energy is used to convert a proton into a neutron, a positron and a neutrino:
energy + p → n + e + νe
So, unlike beta minus decay, beta plus emission cannot occur in isolation because it requires energy input. That is because the mass of the neutron is greater than the mass of the proton. Beta plus decay can only happen inside nuclei when the absolute value of the binding energy of the daughter nucleus is higher than that of the mother nucleus. The difference between these energies goes into the reaction of converting the particles and into the kinetic energy of these particles. Other than that, the sequence is similar - a mirror image of beta minus decay.
There are more useful pages about different aspects and uses of radioactivity here:
- What is radioactivity
- Properties of alpha, beta and gamma radiation
- Detecting ionising radiation with a geiger counter video
- Beta minus and beta plus notes and video
- Explaining radioactivity half life
- Carbon dating
- Radioactive decay equations
- Measuring radioactivity
- Muon Decay and Relativity
- Neutrons, stability and decay - notes and video
- Feynman diagrams notes and video