Mesons are a class of hadrons composed of a quark–antiquark pair. They are strongly interacting particles and play a crucial role in mediating nuclear forces.
Each meson consists of:
Examples:
| Meson | Quark Composition | Charge |
|---|---|---|
| π⁺ | u d̄ | +1 |
| π⁻ | d ū | −1 |
| π⁰ | (u ū − d d̄)/√2 | 0 |
| K⁺ | u s̄ | +1 |
| K⁰ | d s̄ | 0 |
Mesons have integer spin (0 or 1) and hence obey Bose–Einstein statistics.
Meson masses are generally greater than leptons but less than baryons.
Mesons are generally unstable and decay via strong or weak interactions.
| Type | Examples | Spin |
|---|---|---|
| Pseudoscalar Mesons | π, K, η | 0 |
| Vector Mesons | ρ, ω, φ | 1 |
| Interaction | Participate? |
|---|---|
| Gravitational | Yes |
| Electromagnetic | Charged mesons |
| Weak | Yes |
| Strong | Yes |
Yukawa proposed that nuclear force between nucleons is mediated by pions (π-mesons).
| Property | Mesons | Leptons |
|---|---|---|
| Constituents | Quark + Antiquark | Elementary |
| Strong Interaction | Yes | No |
| Spin | 0 or 1 | 1/2 |