3.2.1.6
There are three quarks you need to know: up, down and strange
Quarks, Leptons & Conservation Laws — AQA A-Level Physics
- Quarks are fundamental particles that combine to form hadrons.
- At A-Level, you need three quarks: up ($u$), down ($d$) and strange ($s$).
- Each quark has a corresponding antiquark with opposite chargeA property of matter that causes it to experience a force in an electromagnetic field. Measured in coulombs (C)., baryon numberA quantum number conserved in all interactions. Baryons (protons, neutrons) have baryon number +1, antibaryons have -1, and mesons/leptons have 0. and strangeness.
Quark properties
| Quark | Symbol | Charge | Baryon Number | Strangeness |
|---|---|---|---|---|
| Up | $u$ | $+\frac{2}{3}$ | $+\frac{1}{3}$ | $0$ |
| Down | $d$ | $-\frac{1}{3}$ | $+\frac{1}{3}$ | $0$ |
| Strange | $s$ | $-\frac{1}{3}$ | $+\frac{1}{3}$ | $-1$ |
| Anti-up | $\bar{u}$ | $-\frac{2}{3}$ | $-\frac{1}{3}$ | $0$ |
| Anti-down | $\bar{d}$ | $+\frac{1}{3}$ | $-\frac{1}{3}$ | $0$ |
| Anti-strange | $\bar{s}$ | $+\frac{1}{3}$ | $-\frac{1}{3}$ | $+1$ |
Quark composition of common particles
| Particle | Symbol | Quark Content | Charge | Strangeness |
|---|---|---|---|---|
| Proton | $p$ | $uud$ | $+1$ | $0$ |
| Neutron | $n$ | $udd$ | $0$ | $0$ |
| Pion + | $\pi^{+}$ | $u\bar{d}$ | $+1$ | $0$ |
| Pion − | $\pi^{-}$ | $\bar{u}d$ | $-1$ | $0$ |
| Pion 0 | $\pi^{0}$ | $u\bar{u}$ or $d\bar{d}$ | $0$ | $0$ |
| Kaon + | $K^{+}$ | $u\bar{s}$ | $+1$ | $+1$ |
| Kaon − | $K^{-}$ | $\bar{u}s$ | $-1$ | $-1$ |
| Kaon 0 | $K^{0}$ | $d\bar{s}$ | $0$ | $+1$ |
Common Mistake
MEDIUM
Students often: Assigning strangeness $= +1$ to the strange quark.
Instead: The strange quark has strangeness $= -1$. The anti-strange quark has strangeness $= +1$. Particles containing $s$ have $S = -1$ (e.g. $K^{-}$, $\Lambda^{0}$). Particles containing $\bar{s}$ have $S = +1$ (e.g. $K^{+}$).
Instead: The strange quark has strangeness $= -1$. The anti-strange quark has strangeness $= +1$. Particles containing $s$ have $S = -1$ (e.g. $K^{-}$, $\Lambda^{0}$). Particles containing $\bar{s}$ have $S = +1$ (e.g. $K^{+}$).
Related:Particle Interactions