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Omega baryon
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Bluestar Bluestar Bluestar Bluestar Blackstar

Omega baryons (often called simply omega particles) are a family of subatomic which are represented by the symbol and are either charge or have a +2, +1 or −1 elementary charge. Additionally, they contain no or . Omega baryons containing are also not expected to be observed. This is because the predicts the of top quarks to be roughly , which is about a twentieth of the timescale necessary for the strong interactions required for , the process by which hadrons form from quarks and gluons.

The earliest observed omega baryon was the , made of three . It was first observed in 1964. The discovery was a great triumph in the study of , since it was found only after its existence, mass, and decay products had been predicted in 1961 by the and, independently, by the Yuval Ne'eman. A charmed omega particle () was discovered in 1985, in which a strange quark is replaced by a . The decays only via the weak interaction and therefore has a relatively long lifetime. Spin ( J) and parity ( P) values for unobserved baryons are predicted by the .

Since omega baryons do not have any up or down quarks, they all have 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
+Omega
Omega +−1−300 or
or

Charmed omega +0−2+10 See Decay Modes
Bottom omega +−1−20−1 (seen)
Double charmed omega† ++1−1+20
Charmed bottom omega† +0−1+1−1
Double bottom omega† +−1−10−2
Triple charmed omega† ++20+30
Double charmed bottom omega† ++10+2−1
Charmed double bottom omega† +00+1−2
Triple bottom omega† +−100−3
† Particle (or quantity, i.e. spin) has neither been observed nor indicated.


Recent discoveries
The particle is a "doubly " containing two strange quarks and a . A discovery of this particle was first claimed in September 2008 by physicists working on the experiment at the facility of the Fermi National Accelerator Laboratory. However, the reported mass of was significantly higher than expected in the . The apparent discrepancy from the has since been dubbed the " puzzle". In May 2009, the CDF collaboration made public their results on the search for the based on analysis of a data sample roughly four times the size of the one used by the DØ experiment. CDF measured the mass to be , which was in excellent agreement with the Standard Model prediction. No signal has been observed at the DØ reported value. The two results differ by , which is equivalent to 6.2 standard deviations and are therefore inconsistent. Excellent agreement between the CDF measured mass and theoretical expectations is a strong indication that the particle discovered by CDF is indeed the . In February 2013 the collaboration published a measurement of the mass that is consistent with, but more precise than, the CDF result.

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.


See also


External links

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