Represent α‑ and β‑decay by a radioactive decay equation of the form $\,_{Z}^{A}\text{X} \rightarrow \,_{Z'}^{A'}\text{Y} + \text{particle}\,$.
In α‑decay the nucleus emits an α‑particle, which is a helium‑4 nucleus:
$$ \,_{92}^{238}\text{U} \;\rightarrow\; \,_{90}^{234}\text{Th} \;+\; \,_{2}^{4}\alpha $$In β‑decay a neutron is transformed into a proton with the emission of an electron (β⁻ particle) and an antineutrino (often omitted in simple equations):
$$ \,_{6}^{14}\text{C} \;\rightarrow\; \,_{7}^{14}\text{N} \;+\; \,_{-1}^{0}\beta $$| Feature | α‑Decay | β‑Decay |
|---|---|---|
| Particle emitted | α‑particle ($\,_{2}^{4}\alpha$) | β⁻ particle ($\,_{-1}^{0}\beta$) |
| Change in mass number (A) | ‑4 | 0 |
| Change in atomic number (Z) | ‑2 | +1 |
| Typical energy released | \overline{4}–9 MeV | \overline{0}.5–2 MeV |