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The quark model explains the internal structure of hadrons (protons, neutrons, pions, and many other particles). It was proposed independently by Murray Gell-Mann and George Zweig in 1964 and is a cornerstone of the Standard Model of particle physics. This lesson covers quarks, antiquarks, hadrons, baryons, mesons, and the quantum numbers used to classify particles. This is assessed in AQA section 3.2.1.
Quarks are fundamental particles — they have no known internal structure. At A-Level, you need to know three flavours (types) of quark:
| Quark | Symbol | Charge (e) | Baryon number (B) | Strangeness (S) |
|---|---|---|---|---|
| Up | u | +⅔ | +⅓ | 0 |
| Down | d | −⅓ | +⅓ | 0 |
| Strange | s | −⅓ | +⅓ | −1 |
Every quark has a corresponding antiquark with the opposite charge, opposite baryon number, and opposite strangeness:
| Antiquark | Symbol | Charge (e) | Baryon number (B) | Strangeness (S) |
|---|---|---|---|---|
| Anti-up | ū | −⅔ | −⅓ | 0 |
| Anti-down | d̄ | +⅓ | −⅓ | 0 |
| Anti-strange | s̄ | +⅓ | −⅓ | +1 |
Key Point: Every quantum number of an antiquark is the exact negative of the corresponding quark. So if the strange quark has strangeness −1, the anti-strange quark has strangeness +1.
Hadrons are particles made of quarks. They feel the strong nuclear force. Hadrons are divided into two families:
Baryons are made of three quarks (qqq). They have baryon number B = +1 (since each quark contributes +⅓).
| Baryon | Quark composition | Charge (e) | Strangeness |
|---|---|---|---|
| Proton (p) | uud | +⅔ +⅔ −⅓ = +1 | 0 |
| Neutron (n) | udd | +⅔ −⅓ −⅓ = 0 | 0 |
| Sigma-plus (Σ⁺) | uus | +⅔ +⅔ −⅓ = +1 | −1 |
| Sigma-zero (Σ⁰) | uds | +⅔ −⅓ −⅓ = 0 | −1 |
| Sigma-minus (Σ⁻) | dds | −⅓ −⅓ −⅓ = −1 | −1 |
| Xi-minus (Ξ⁻) | dss | −⅓ −⅓ −⅓ = −1 | −2 |
| Omega-minus (Ω⁻) | sss | −⅓ −⅓ −⅓ = −1 | −3 |
Antibaryons are made of three antiquarks (q̄q̄q̄). They have baryon number B = −1.
Mesons are made of one quark and one antiquark (qq̄). They have baryon number B = 0 (since +⅓ and −⅓ cancel).
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