Before you can read the parent note Radioactive decay — alpha, beta, gamma — mechanisms, you must own every symbol it throws at you. This page builds each one from nothing — plain words, then a picture, then why the topic needs it. Read top to bottom; every idea leans on the one above it.
Picture a nucleus as a tight little cluster of balls. Some balls are protons (they carry positive electric charge), and some are neutrons (they carry no charge — they are electrically neutral, hence the name).
Picture: count the magenta balls in the figure above — that count is Z.
Why the topic needs it: Z decides which element you are. Z=6 is always carbon, Z=92 is always uranium. When a decay changes Z, the atom turns into a different element. Charge conservation (rule 1 of the parent note) is really "the total Z on the left equals the total Z on the right."
Picture: count all the balls, magenta and violet — that total is A.
Why the topic needs it: A tracks the "bulk" of the nucleus. When a chunk is thrown out (alpha decay), A drops. When a neutron just flips into a proton (beta decay), A stays the same because you still have the same number of balls. Nucleon-number conservation (rule 2) says the total A can never change across the arrow.
These are just names, borrowed from the Greek alphabet, for the three kinds of "stuff" a nucleus emits — labelled in the historical order they were discovered (first, second, third letter).
Why the topic needs them: these four symbols are the entire cast of decay products. Every decay equation in the parent note is built from X, Y, and one of α,β,γ,ν.
a bare e inside "+2e" or "−e" means the size of one proton's charge — a unit of charge, not a particle.
So "the alpha has charge +2e" means "twice the proton charge," because an alpha holds 2 protons. The topic needs this because charge is measured in multiples of e, and that is how the comparison table lists charges.
Why the topic needs it: the parent note claims "products are lighter than the parent, and the missing mass becomes kinetic energy." That sentence is only meaningful because of E=mc2 — missing mass is released energy. This is the same idea explored in Nuclear binding energy and mass defect.
Picture: put the parent on one pan of a scale and all its products on the other. If the products are lighter, that missing weight — times c2 — is the energy handed out as motion.
Why the topic needs it: Q is the single number that answers "will it decay, and how much energy comes out?" Every worked example computes kinetic energies as fractions of Q.
Recall Quick self-check on
Q
If products are heavier than the parent, can the decay happen spontaneously? ::: No — that needs Q>0, i.e. products lighter than parent; heavier products give Q<0.
Why the topic needs it: this single distinction is the fingerprint that separates the decays. Alpha and gamma give discrete lines (two-body split → fixed shares). Beta gives a continuous band, because a third particle (the neutrino) secretly shares the energy differently each time — that continuous shape is the historical clue that forced the neutrino's existence. See Neutrino and lepton number conservation.
You do not need to master these yet, but recognise the names:
Quantum tunnelling — a particle "leaking" through a wall it classically could not cross. This is how an alpha escapes: Quantum tunnelling.
Weak interaction — the fundamental force that flips a neutron into a proton (and vice-versa) and creates the electron + neutrino. This is how beta decay happens: Weak interaction.