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In the last lesson we met the Standard Model in outline: quarks and leptons as the fundamental fermions, gauge bosons as force carriers, and the Higgs boson providing mass. In this lesson we dig into the quark and lepton content in more detail, and show how quarks combine into hadrons — the composite particles built from them, including the familiar protons and neutrons.
This is the heart of section 6.4.4 of the OCR A-Level Physics A specification (H556), and it introduces the terminology (baryons, mesons, baryon number, lepton number) you will need for Lesson 9 on conservation rules.
Quarks are point-like, fundamental particles that experience the strong nuclear force. There are six types (or "flavours"), organised into three generations:
| Flavour | Symbol | Charge (e) | Mass (MeV/c²) | Generation |
|---|---|---|---|---|
| Up | u | +2/3 | ~2.2 | 1st |
| Down | d | -1/3 | ~4.7 | 1st |
| Charm | c | +2/3 | ~1270 | 2nd |
| Strange | s | -1/3 | ~95 | 2nd |
| Top | t | +2/3 | ~173000 | 3rd |
| Bottom | b | -1/3 | ~4180 | 3rd |
The OCR specification focuses on just the first three: up, down and strange. You should know their charges and that they are classified as fundamental.
Some crucial properties:
+2/3 e or -1/3 e.u is ū with charge -2/3; the antiparticle of d is d̄ with charge +1/3; and so on.B = +1/3 (antiquarks have B = -1/3).Leptons are point-like particles that do not feel the strong nuclear force. Like quarks, there are six of them, in three generations:
| Lepton | Symbol | Charge (e) | Mass (MeV/c²) |
|---|---|---|---|
| Electron | e⁻ | -1 | 0.511 |
| Electron neutrino | ν_e | 0 | ≈ 0 |
| Muon | μ⁻ | -1 | 105.7 |
| Muon neutrino | ν_μ | 0 | ≈ 0 |
| Tau | τ⁻ | -1 | 1777 |
| Tau neutrino | ν_τ | 0 | ≈ 0 |
And again, each has an antiparticle: the antielectron (positron) e⁺, the antimuon μ⁺, the antitau τ⁺, and the three antineutrinos ν̄_e, ν̄_μ, ν̄_τ.
OCR specifies the electron and the muon as examples of leptons, and the electron neutrino and electron antineutrino as particles you must recognise in beta decay equations.
Some important properties:
L = +1; antileptons have L = -1. Lepton number is conserved in all known interactions.μ^- → e^- + ν̄_e + ν_μ, conserving both electron and muon lepton numbers.A hadron is any particle built from quarks. Because quarks cannot exist in isolation, all directly observable particles that feel the strong force are hadrons. There are two main types:
qqq).q\bar{q}).Both combinations are "colourless" (in the technical sense of the colour charge we mentioned earlier) and therefore allowed. Single quarks and quark-quark pairs would not be colourless, so you never see them on their own.
Baryons are hadrons made of three quarks. The most familiar baryons are the proton and neutron, which are made of up and down quarks.
| Baryon | Quark content | Charge | Mass (MeV/c²) |
|---|---|---|---|
| Proton | uud | +1 | 938.3 |
| Neutron | udd | 0 | 939.6 |
Lambda (Λ⁰) | uds | 0 | 1116 |
Sigma (Σ⁺) | uus | +1 | 1189 |
Sigma (Σ⁻) | dds | -1 | 1197 |
Xi (Ξ⁰) | uss | 0 | 1315 |
Check the proton charge:
Q(uud) = (+2/3) + (+2/3) + (-1/3) = +1 ✓
Check the neutron charge:
Q(udd) = (+2/3) + (-1/3) + (-1/3) = 0 ✓
The mechanism works beautifully: fractional quark charges combine to give integer hadron charges.
Baryons have baryon number B = +1. (Three quarks with B = 1/3 each gives B = 1.) Antibaryons have B = -1. Baryon number is conserved in all known interactions — which is why the proton appears to be stable (no lighter baryon exists for it to decay into).
Baryons heavier than nucleons are called hyperons. The \Lambda, \Sigma and \Xi particles are hyperons, all containing at least one strange quark. They decay to lighter baryons via the weak interaction with lifetimes of order 10^{-10} s.
Mesons are hadrons made of one quark and one antiquark (q\bar{q}). They are bosons (integer spin), unlike baryons (which are fermions with half-integer spin).
| Meson | Quark content | Charge | Mass (MeV/c²) |
|---|---|---|---|
Pion π⁺ | ud̄ | +1 | 139.6 |
Pion π⁻ | ūd | -1 | 139.6 |
Pion π⁰ | uū / dd̄ | 0 | 135.0 |
Kaon K⁺ | us̄ | +1 | 493.7 |
Kaon K⁻ | ūs | -1 | 493.7 |
Kaon K⁰ | ds̄ | 0 | 497.6 |
Check the π⁺ charge:
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