The Xi baryons or cascade particles are a family of subatomic hadron particles which have the symbol Ξ and may have an electric charge (Q) of +2 e, +1 e, 0, or −1 e, where e is the elementary charge.
| Composition |
|
|---|---|
| Statistics | Fermionic |
| Family | Baryons |
| Interactions | Strong, weak, electromagnetic, and gravity |
| Types | 2 |
| Mass | |
| Spin | 1⁄2 |
| Strangeness | -2 |
| Isospin | 1⁄2 |
Like all conventional baryons, Ξ particles contain three quarks. Ξ baryons, in particular, contain either one up or one down quark and two other, more massive quarks. The two more massive quarks are any two of strange, charm, or bottom (doubles allowed). For notation, the assumption is that the two heavy quarks in the Ξ are both strange; subscripts "c" and "b" are added for each even heavier charm or bottom quark that replaces one of the two presumed strange quarks.
They are historically called the cascade particles because of their unstable state; they are typically observed to decay rapidly into lighter particles, through a chain of decays (cascading decays).[2] The first discovery of a charged Xi baryon was in cosmic ray experiments by the Manchester group in 1952.[3] The first discovery of the neutral Xi particle was at Lawrence Berkeley Laboratory in 1959.[4] It was also observed as a daughter product from the decay of the omega baryon (
Ω−
) observed at Brookhaven National Laboratory in 1964.[2] The Xi spectrum is important to nonperturbative quantum chromodynamics (QCD), such as lattice QCD.[why?]
History
The
Ξ−
b particle is also known as the cascade B particle and contains quarks from all three families. It was discovered by DØ and CDF experiments at Fermilab. The discovery was announced on 12 June 2007. It was the first known particle made of quarks from all three quark generations – namely, a down quark, a strange quark, and a bottom quark. The DØ and CDF collaborations reported the consistent masses of the new state. The Particle Data Group world average mass is 5.7924±0.0030 GeV/c2.
For notation, the assumption is that the two heavy quarks are both strange, denoted by a simple Ξ ; a subscript "c" is added for each constituent charm quark, and a "b" for each bottom quark. Hence Ξc, Ξb, Ξcc, Ξcb, etc.
Unless specified, the non-up/down quark content of Xi baryons is strange (i.e. there is one up or down quark and two strange quarks). However a
Ξ0
b contains one up, one strange, and one bottom quark, while a
Ξ0
bb contains one up and two bottom quarks.
In 2012, the CMS experiment at the Large Hadron Collider detected a
Ξ∗0
b baryon (reported mass 5945±2.8 MeV/c2).[5][6] (Here,"*" indicates a baryon decuplet.) The LHCb experiment at CERN discovered two new Xi baryons in 2014:
Ξ′−
b and
Ξ∗−
b.[7]
In 2017, the LHCb researchers reported yet another Xi baryon: the double charmed
Ξ++
cc baryon, consisting of two heavy charm quarks and one up quark. The mass of
Ξ++
cc is about 3.8 times that of a proton.[8][9]
List of Xi baryons
Isospin and spin values in parentheses have not been firmly established by experiments, but are predicted by the quark model and are consistent with the measurements.
| Particle | Symbol | Makeup | Rest mass (MeV/c2) |
Isospin, I |
Spin, parity, JP |
Q | S | C | B | Mean lifetime (s) |
Decays to |
|---|---|---|---|---|---|---|---|---|---|---|---|
| Xi[14] | Ξ0 |
u s s |
1314.86±0.20 | 1/2 | 1/2(+) | 0 | −2 | 0 | 0 | (2.90±0.09)×10−10 | Λ0 + π0 |
| Xi[15] | Ξ− |
d s s |
1321.71±0.07 | 1/2 | 1/2(+) | −1 | −2 | 0 | 0 | (1.639±0.015)×10−10 | Λ0 + π− |
| Xi resonance[16] | Ξ0 (1530) |
u s s |
1531.80±0.32 | 1/2 | 3/2+ | 0 | −2 | 0 | 0 | (7.2±0.4)×10−23[lower-alpha 1] | Ξ + π |
| Xi resonance[16] | Ξ− (1530) |
d s s |
1535.0±0.6 | 1/2 | 3/2+ | −1 | −2 | 0 | 0 | 6.6+1.6 −1.0×10−23[lower-alpha 1] |
Ξ + π |
| charmed Xi[17] | Ξ+ c |
u s c |
2467.9±0.4 | 1/2 | (1/2 +) | +1 | −1 | +1 | 0 | (4.42±0.26)×10−13 | See Ξ+ c decay modes |
| charmed Xi[17] | Ξ0 c |
d s c |
2471.0±0.4 | 1/2 | (1/2 +) | 0 | −1 | +1 | 0 | 1.12+0.13 −0.10×10−13 |
See Ξ0 c decay modes |
| charmed Xi resonance[17] | Ξ′+ c |
u s c |
2575.7±3.1 | 1/2 | (1/2+) | +1 | −1 | +1 | 0 | Ξ+ c + γ (Seen) | |
| charmed Xi resonance[17] | Ξ′0 c |
d s c |
2578.0±2.9 | 1/2 | (1/2+) | 0 | −1 | +1 | 0 | Ξ0 c + γ (Seen) | |
| double charmed Xi[8] | Ξ++ cc |
u c c |
3621.40±0.72 ± 0.27 ± 0.14 | (1/2) | (1/2 +) | +2 | 0 | +2 | 0 | 0.256+0.024 −0.022 ±0.014×10−12[18] |
Λ+ c + K− + π+ + π+ |
| double charmed Xi[lower-alpha 2][19] | Ξ+ cc |
d c c |
3518.9±0.9[lower-alpha 2] | (1/2) | (1/2 +) | +1 | 0 | +2 | 0 | <3.3×10−14[lower-alpha 2] | Λ+ c + K− + π+ [e] or p+ + D+ + K− [e] |
| bottom Xi[20] | Ξ0 b |
u s b |
5792±3 | (1/2) | (1/2 +) | 0 | −1 | 0 | −1 | 1.42+0.28 −0.24×10−12[lower-alpha 3] |
See Ξ b decay modes |
| bottom Xi or Cascade B[10][13][20] |
Ξ− b |
d s b |
5792.9±3.0 | (1/2) | (1/2 +) | −1 | −1 | 0 | −1 | 1.42×10−12 | See Ξ b decay modes ( Ξ− + J/ψ was also seen) |
| Ξ′− b[21] |
d s b |
5935.02±0.02 ± 0.01 ± 0.50 | 1/2+ | −1 | −1 | 0 | −1 | >8×10−21[lower-alpha 2][lower-alpha 1] | |||
| Ξ∗− b[21] |
d s b |
5955.33±0.12 ± 0.06 ± 0.50 | 3/2+ | −1 | −1 | 0 | −1 | (3.99±0.75 ± 0.25)×10−22[lower-alpha 1] | |||
| Ξ b(6227)−[22] |
d s b |
6226.9±2.0 ± 0.3 ± 0.2 | −1 | −1 | 0 | −1 | 3.64+1.55 −0.84 ±0.36×10−23[lower-alpha 1] |
Λ b + K− Ξ0 b + π− | |||
| double bottom Xi[lower-alpha 4] | Ξ0 bb |
u b b |
(1/2) | (1/2 +) | 0 | 0 | 0 | −2 | |||
| double bottom Xi[lower-alpha 4] | Ξ− bb |
d b b |
(1/2) | (1/2 +) | −1 | 0 | 0 | −2 | |||
| charmed bottom Xi[lower-alpha 4] | Ξ+ cb |
u c b |
(1/2) | (1/2) + | +1 | 0 | +1 | −1 | |||
| charmed bottom Xi[lower-alpha 4] | Ξ0 cb |
d c b |
(1/2) | (1/2 +) | 0 | 0 | +1 | −1 |
- Table notes
See also
References
External links
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