| Composition | ω: |
|---|---|
| Statistics | Bosonic |
| Family | Mesons |
| Interactions | Strong,weak,electromagnetic,gravity |
| Symbol | ω |
| Antiparticle | Self |
| Theorized | Yoichiro Nambu[1] (1957) |
| Discovered | Lawrence Berkeley National Laboratory (1961)[2][3] |
| Types | 1 |
| Mass | 782.66±0.13 MeV/c2 |
| Mean lifetime | (7.58±0.11)×10−23 s |
| Decays into | π+ +π0 +π− orπ0 +γ |
| Electric charge | 0e |
| Spin | 1 |
| Isospin | 0 |
| Hypercharge | 0 |
| Parity | −1 |
| C parity | −1 |
Theomega meson (ω) is aflavourlessmeson formed from asuperposition of anup quark–antiquark and adown quark–antiquark pair. It is part of thevector meson nonet[4][5] and mediates thenuclear force along withpions andrho mesons.
The most common decay mode for the ω meson isπ+
π0
π−
at89.2%±0.7%, followed byπ0
γ at8.34%±0.26%.[6]
| Particle name | Particle symbol | Antiparticle symbol | Quark content | Rest mass (MeV/c2) | IG | JPC | S | C | B' | Mean lifetime (s) | Commonly decays to (>5% of decays) |
|---|---|---|---|---|---|---|---|---|---|---|---|
| Omega meson[6] | ω(782) | Self | 782.66 ± 0.13 | 0− | 1−− | 0 | 0 | 0 | (7.58±0.11)×10−23 s | π+ +π0 +π− or π0 +γ |
The quark composition of theω meson can be thought of as a mix betweenuu,dd andss states, but it is very nearly a pure symmetricuu–dd state. This can be shown by deconstructing thewave function of theω into its component parts. We see that theω andϕ mesons are mixtures of theSU(3) wave functions as follows.[7]
where
The mixing angle at which the components decouple completely can be calculated to be, which almost corresponds to the actual value calculated from the masses of 35°. Therefore, theω meson is nearly a pure symmetricuu–dd state.