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Omega baryon
Subatomic hadron particle
Subatomic hadron particle
Omega baryons (often called simply omega particles) are a family of subatomic hadrons which are represented by the symbol and are either charge neutral or have a +2, +1 or −1 elementary charge. Additionally, they contain no up or down quarks. Omega baryons containing top quarks are also not expected to be observed. This is because the Standard Model predicts the mean lifetime of top quarks to be roughly , |url-access=subscription
The earliest observed omega baryon was the , made of three strange quarks. It was first observed in 1964. |display-authors=etal}} The discovery was a great triumph in the study of quarks, since it was found only after its existence, mass, and decay products had been predicted in 1961 by the American physicist Susumu Okubo and independently Murray Gell-Mann in a less accurate formula. A charmed omega particle () was discovered in 1985, in which a strange quark is replaced by a charm quark. The decays only via the weak interaction and therefore has a relatively long lifetime. |access-date=2009-11-26
Since omega baryons do not have any up or down quarks, they all have isospin 0.
The naming convention of baryons has become such that those with no light (i.e. up or down) valence quarks are called omega baryons. By default, the quarks are strange quarks, but those with one or more the strange quarks replaced by charm or bottom quarks have a subscript c or b, respectively.
Omega baryons
| Particle | Symbol | Quark | ||||||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| content | Rest mass | |||||||||||||
| (MeV/*c*2) | JP | Q | ||||||||||||
| (*e*) | S | C | B' | Mean lifetime | ||||||||||
| (s) | Decays to | |||||||||||||
| author=Particle Data Group | author-link=Particle Data Group | url=http://pdg.lbl.gov/2007/listings/s024.pdf | title= 2006 Review of Particle Physics – | access-date=2008-04-20 }} | + | −1 | −3 | 0 | 0 | or | ||||
| or | ||||||||||||||
| author=Particle Data Group | author-link=Particle Data Group | url=http://pdg.lbl.gov/2018/listings/rpp2018-list-omegac-zero.pdf | title= listing – | access-date=13 August 2018 }} | + | 0 | −2 | +1 | 0 | See [ Decay Modes](https://pdg.lbl.gov/2022/listings/contents_listings.html) | ||||
| Bottom omega | + | −1 | −2 | 0 | −1 | (seen) | ||||||||
| Double charmed omega† | + | +1 | −1 | +2 | 0 | |||||||||
| Charmed bottom omega† | + | 0 | −1 | +1 | −1 | |||||||||
| Double bottom omega† | + | −1 | −1 | 0 | −2 | |||||||||
| Triple charmed omega† | + | +2 | 0 | +3 | 0 | |||||||||
| Double charmed bottom omega† | + | +1 | 0 | +2 | −1 | |||||||||
| Charmed double bottom omega† | + | 0 | 0 | +1 | −2 | |||||||||
| Triple bottom omega† | + | −1 | 0 | 0 | −3 |
† Particle (or quantity, i.e. spin) has neither been observed nor indicated. m_W + m_b ***** ---
Recent discoveries
The particle is a "doubly strange" baryon containing two strange quarks and a bottom quark. A discovery of this particle was first claimed in September 2008 by physicists working on the DØ experiment at the Tevatron facility of the Fermi National Accelerator Laboratory. |access-date=2008-09-04
In March 2017, the LHCb collaboration announced the observation of five new narrow states decaying to , where the was reconstructed in the decay mode . The states are named (3000)0, (3050)0, (3066)0, (3090)0 and (3119)0. Their masses and widths were reported, but their quantum numbers could not be determined due to the large background present in the sample.
References
References
- Particle Data Group. "2010 Review of Particle Physics – Naming scheme for hadrons".
- (1994-01-01). "Heavy baryons". Progress in Particle and Nuclear Physics.
- Particle Data Group. "2006 Review of Particle Physics – {{SubatomicParticle".
- Particle Data Group. "{{SubatomicParticle".
- "LHCb observes an exceptionally large group of particles". CERN.
- R. Aaij ''et al.'' ([[LHCb. (2017). "Observation of five new narrow {{SubatomicParticle". Physical Review Letters.
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