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Xi baryon
please note:
- the content below is remote from Wikipedia
- it has been imported raw for GetWiki
{{Short description|Subatomic particle}}- the content below is remote from Wikipedia
- it has been imported raw for GetWiki
factoids | |||||||||||||||||||||||||||
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name | Xi baryon| num_types = 2
| Strong interaction>Strong, Weak interaction | , Electromagnetic interaction>electromagnetic, and gravity| antiparticle = | status = | theorized = | discovered = | symbol = |
| 1|2}}| num_spin_states = | baryon_number = | strangeness = -2| charm = | bottomness = | topness = | 1|2}}| weak_isospin = | weak_isospin_3 = | hypercharge = | weak_hypercharge = | chirality = | B-L =| X_charge =| parity = | g_parity = | c_parity = | r_parity = | condensed_symmetries =}}The Xi baryons or cascade particles are a family of subatomic hadron particles which have the symbol {{math|Î}} and may have an electric charge ({{mvar|Q}}) of +2 {{mvar|e}}, +1 {{mvar|e}}, 0, or â1 {{mvar|e}}, where {{mvar|e}} is the elementary charge.Like all conventional baryons, {{math|Î}} particles contain three quarks. {{math|Î}} 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 {{math|Î}} 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).WEB
,
The first discovery of a charged Xi baryon was in cosmic ray experiments by the Manchester group in 1952.
JOURNAL
, R., Armenteros , , etal , Manchester group , 1952 , The properties of charged V-particles , Philosophical Magazine , 43, 341, 597 , 10.1080/14786440608520216
The first discovery of the neutral Xi particle was at Lawrence Berkeley Laboratory in 1959.
JOURNAL
, L.W., Alvarez , , etal , 1959 , Neutral Cascade Hyperon Event , Physical Review Letters , 2, 5, 215 , 1959PhRvL...2..215A, 10.1103/PhysRevLett.2.215 ,weblink
It was also observed as a daughter product from the decay of the omega baryon ({{math|{{SubatomicParticle|Omega-}}}}) observed at Brookhaven National Laboratory in 1964. The Xi spectrum is important to nonperturbative quantum chromodynamics (QCD), such as lattice QCD.{{why|date=December 2016}}
HistoryThe {{math|{{SubatomicParticle|Bottom Xi-}}}} particle is also known as the cascade B particle and contains quarks from all three families. It was discovered by DÃ 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 â namely, a down quark, a strange quark, and a bottom quark. The DÃ and CDF collaborations reported the consistent masses of the new state. The Particle Data Group world average mass is {{val|5.7924|0.0030|u=GeV/c2}}.For notation, the assumption is that the two heavy quarks are both strange, denoted by a simple {{math|Î}} ; a subscript "c" is added for each constituent charm quark, and a "b" for each bottom quark. Hence {{math|Î}}{{sub|c}}, {{math|Î}}{{sub|b}}, {{math|Î}}{{sub|cc}}, {{math|Î}}{{sub|cb}}, 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 {{math|{{SubatomicParticle|Bottom Xi0}}}} contains one up, one strange, and one bottom quark, while a {{math|{{SubatomicParticle|Double bottom xi0}}}} contains one up and two bottom quarks.In 2012, the CMS experiment at the Large Hadron Collider detected a {{math|{{SubatomicParticle|bottom xi*0}}}} baryon (reported mass {{val|5945|2.8|u=MeV/c2}}).WEB, C., Simpson , JOURNAL
, 28 April 2013 , New particle discovered with 'Higgs boson' machine , The Atlantic Wire ,weblink , 2013-04-04 , S., Chatrchyan
PRESS RELEASE
, etal , Compact Muon Solenoid, CMS Collaboration , 2012 , Observation of a new Îb baryon , Physical Review Letters , 108, 25, 252002 , 1204.5955, 2012PhRvL.108y2002C, 23004588 , 10.1103/PhysRevLett.108.252002, 119204847 , (Here,"*" indicates a baryon decuplet.) The LHCb experiment at CERN discovered two new Xi baryons in 2014: {{math|{{Subatomic particle|bottom xi'-}}}} and {{math|{{Subatomic particle|bottom xi*-}}}}. , LHCb experiment observes two new baryon particles never seen before , In 2017, the LHCb researchers reported yet another Xi baryon: the double charmed {{math| {{SubatomicParticle|Double charmed Xi++}} }} baryon, consisting of two heavy charm quarks and one up quark. The mass of {{math|{{SubatomicParticle|Double charmed Xi++}}}} is about 3.8 times that of a proton.PRESS RELEASE
, 19 November 2014 , CERN , Bern, CH ,weblink , The LHCb experiment is charmed to announce observation of a new particle with two heavy quarks , NEWS
, 2017-07-06 , CERN ,weblink , 2017-07-06 , Chang, Kenneth , , 2017-07-06 , CERN physicists find a particle with a double dose of charm , The New York Times , en-US, 0362-4331 ,weblink , 2017-07-08 List of Xi baryonsIsospin 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.{| class="wikitable sortable"|+ Xi baryonsJOURNAL, V., Abazov
}}PRESS RELEASE
, PRESS RELEASE
, JOURNAL
, etal , D0 experiment, D0 Collaboration , 2007 , Direct observation of the strange b baryon {{math, {{SubatomicParticle, Bottom Xi-, }} |journal=Physical Review Letters |volume=99 |issue=5 |pages=52001 |arxiv=0706.1690 |bibcode=2007PhRvL..99e2001A |doi=10.1103/PhysRevLett.99.052001 |pmid=17930744 |hdl=10211.3/194385 |s2cid=11568965 , T., Aaltonen
}}, etal , Collider Detector at Fermilab, CDF Collaboration , 2007 , Observation and mass measurement of the baryon Î{{su, b, −, |journal=Physical Review Letters |volume=99 |issue=5 |page=52002 |arxiv=0707.0589 |bibcode=2007PhRvL..99e2002A |s2cid=45025038 |pmid=17930745 |hdl=10261/8530 |doi=10.1103/PhysRevLett.99.052002 | |||||||||||||||||||||
{{math | Xi0}} }} | {{math | link=yes | link=yes | link=yes|Strange quark}} }} | {{val | 0.20}} | {{sfrac | 2}} | {{sfrac | 2}}(+) | 0 | â2 | 0 | 0 | {{val | 0.09|e=-10}} | {{math | {{SubatomicParticle | Lambda0}} + {{SubatomicParticle | Pion0}}}} }} | ||||||
{{math | Xi-}} }} | {{math | link=yes | link=yes | link=yes|Strange quark}} }} | {{val | 0.07}} | {{sfrac | 2}} | {{sfrac | 2}}(+) | â1 | â2 | 0 | 0 | {{val | 0.015|e=-10}} | {{math | {{SubatomicParticle | Lambda0}} + {{SubatomicParticle | Pion-}} }} }} | ||||||
{{math | Xi0}}}}(1530) | {{math | link=yes | link=yes | link=yes|Strange quark}} }} | {{val | 0.32}} | {{sfrac | 2}} | {{sfrac | 2}}+ | 0 | â2 | 0 | 0 | {{val | 0.4 | name="decaywidth" | Î}}) was reported for this species. Here the conversion {{mvar | ħ|Î}} }} is given instead.}} | {{math | {{SubatomicParticle | Xi}} + {{SubatomicParticle | Pion}} }} }} | |||
{{math | Xi-}}}}(1530) | {{math | link=yes | link=yes | link=yes|Strange quark}} }} | {{val | 0.6}} | {{sfrac | 2}} | {{sfrac | 2}}+ | â1 | â2 | 0 | 0 | {{val | 1.6 | e=-23}}{{efn|name="decaywidth"}} | {{math | {{SubatomicParticle | Xi}} + {{SubatomicParticle | Pion}} }} }} | |||||
{{math | Charmed Xi+}} }} | {{math | link=yes | link=yes | link=yes|Charm quark}} }} | {{val | 0.4}} | {{sfrac | 2}} | ({{sfrac | 2}}{{thinsp}}+) | +1 | â1 | +1 | 0 | {{val | 0.26|e=-13}} | See {{math | charmed Xi+}} }}decay modes | ||||||||
{{math | Charmed Xi0}} }} | {{math | link=yes | link=yes | link=yes|Charm quark}} }} | {{val | 0.4}} | {{sfrac | 2}} | ({{sfrac | 2}}{{thinsp}}+) | 0 | â1 | +1 | 0 | {{val | +0.13 | e=-13}} | See {{math | charmed Xi0}} }}decay modes | |||||||
{{math | Charmed xi'+}} }} | {{math | link=yes | link=yes | link=yes|Charm quark}} }} | {{val | 3.1}} | {{sfrac | 2}} | ({{sfrac | 2}}+) | +1 | â1 | +1 | 0 | {{math | {{SubatomicParticle | Photon}} }}(Seen)}} | |||||||||
{{math | Charmed xi'0}} }} | {{math | link=yes | link=yes | link=yes|Charm quark}} }} | {{val | 2.9}} | {{sfrac | 2}} | ({{sfrac | 2}}+) | 0 | â1 | +1 | 0 | {{math | {{math | Charmed xi0}} + {{SubatomicParticle|Photon}}}} }}(Seen)}} | |||||||||
Îcc++>double charmed Xi | {{math | Double charmed Xi++}} }} | {{math | link=yes | link=yes | link=yes|Charm quark}} }} | {{val | 0.72|errend= ± 0.27 ± 0.14}} | ({{sfrac | 2}}) | ({{sfrac | 2}}{{thinsp}}+) | +2 | 0 | +2 | 0 | 0.256{{SubSup | â0.022|+0.024}}±0.014Ã10â12WEB , | {{math | {{SubatomicParticle | Charmed lambda+}} + {{SubatomicParticle | Kaon-}} + {{SubatomicParticle | Pion+}} + {{SubatomicParticle | Pion+}} }} }} | |||
name="dispute"|Some controversy exists about this data. See references}}JOURNAL
, W.-M., Yao
}}, etal , Particle Data Group , 2006 , Particle listings â Î{{su, +, cc, |url=http://pdg.lbl.gov/2007/listings/s065.pdf |journal=Journal of Physics G |volume=33 |issue=1 |page=1 |arxiv= astro-ph/0601168 |bibcode= 2006JPhG...33....1Y |doi= 10.1088/0954-3899/33/1/001 | {{math | Double charmed Xi+}} }} | {{math | link=yes | link=yes | link=yes|Charm quark}} }} | {{val | 0.9}}{{efn|name="dispute"}} | ({{sfrac | 2}}) | ({{sfrac | 2}}{{thinsp}}+) | +1 | 0 | +2 | 0 | <{{val | e=-14}}{{efn|name="dispute"}} | {{math | {{SubatomicParticle | Charmed lambda+}} + {{SubatomicParticle | Kaon-}} + {{SubatomicParticle | Pion+}}}}}}[e] or {{math | {{SubatomicParticle | Proton+}} + {{SubatomicParticle | D+}} + {{SubatomicParticle | Kaon-}}}}}}[e] |
{{math | Bottom Xi0}} }} | {{math | link=yes | link=yes | link=yes|Bottom quark}} }} | {{val | 3}} | ({{sfrac | 2}}) | ({{sfrac | 2}}{{thinsp}}+) | 0 | â1 | 0 | â1 | {{val | +0.28 | e=-12}}{{efn | This is actually a measurement of the average lifetime of b-baryons that decay to a jet containing a same-sign {{math | Xi}}± {{SubatomicParticle | {{SubatomicParticle | {{SubatomicParticle|Bottom lambda}}.}} }} | See {{math | Bottom Xi}} }}decay modes | |||
{{math | Bottom Xi-}} }} | {{math | link=yes | link=yes | link=yes|Bottom quark}} }} | {{val | 3.0}} | ({{sfrac | 2}}) | ({{sfrac | 2}}{{thinsp}}+) | â1 | â1 | 0 | â1 | {{val | e=-12}} | See {{math | Bottom Xi}} }}decay modes ({{math | {{SubatomicParticle | link=yes|J/Psi}} }} }} was also seen) | ||||||
{{math | Bottom Xi'-}}}}JOURNAL
, Aaij, R.
}}, etal , LHCb Collaboration , 2015 , Observation of two new {{math, Î, {{su|p=â|b=b}} baryon resonances |journal = Physical Review Letters |volume = 114 |issue = 6 |pages = 062004 |doi =10.1103/PhysRevLett.114.062004 |pmid = 25723210 |bibcode = 2015PhRvL.114f2004A |s2cid = 6055559 |arxiv = 1411.4849 | {{math | link=yes | link=yes | link=yes|Bottom quark}} }} | {{val | 0.02|errend= ± 0.01 ± 0.50}} | 1/2+ | â1 | â1 | 0 | â1 | >{{val | e=-21}}{{efn | name="decaywidth"}} | ||||||||||||
{{math | Bottom Xi*-}}}} | {{math | link=yes | link=yes | link=yes|Bottom quark}} }} | {{val | 0.12|errend= ± 0.06 ± 0.50}} | 3/2+ | â1 | â1 | 0 | â1 | {{val | 0.75 | errend= ± 0.25}}{{efn|name="decaywidth"}} | ||||||||||||
{{math | Bottom Xi}}}}(6227)âJOURNAL
, 1805.09418
}}, Aaij, R. , CMS Collaboration , etal , 2018 , Observation of a new {{math, Î, {{su|b=b|p=â}} resonance |journal = Physical Review Letters |volume = 121 |issue = 72002 |pages = 072002 |doi = 10.1103/PhysRevLett.121.072002 |pmid = 30169090 |bibcode =2018PhRvL.121g2002A |s2cid =52139397 | {{math | link=yes | link=yes | link=yes|Bottom quark}} }} | {{val | 2.0|errend= ± 0.3 ± 0.2}} | â1 | â1 | 0 | â1 | 3.64{{SubSup | â0.84 | name="decaywidth"}} | {{math | Bottom lambda}} + {{SubatomicParticle | {{SubatomicParticle | Pion-}} }} | |||||||||
name="notobservered"|Particle (or quantity, i.e. spin) has neither been observed nor indicated}} | {{math | Double Bottom Xi0}} }} | {{math | link=yes | link=yes | link=yes|Bottom quark}} }} | ({{sfrac | 2}}) | ({{sfrac | 2}}{{thinsp}}+) | 0 | 0 | 0 | â2 | |||||||||||||
name="notobservered"}} | {{math | Double Bottom Xi-}} }} | {{math | link=yes | link=yes | link=yes|Bottom quark}} }} | ({{sfrac | 2}}) | ({{sfrac | 2}}{{thinsp}}+) | â1 | 0 | 0 | â2 | |||||||||||||
name="notobservered"}} | {{math | Charmed bottom Xi+}} }} | {{math | link=yes | link=yes | link=yes|Bottom quark}} }} | ({{sfrac | 2}}) | ({{sfrac | 2}}){{thinsp}}+ | +1 | 0 | +1 | â1 | |||||||||||||
name="notobservered"}} | {{math | Charmed bottom Xi0}} }} | {{math | link=yes | link=yes | link=yes|Bottom quark}} }} | ({{sfrac | 2}}) | ({{sfrac | 2}}{{thinsp}}+) | 0 | 0 | +1 | â1 |
- Table notes:
See also
- Delta baryon
- Hyperon
- Lambda baryon
- List of baryons
- List of mesons
- List of particles
- Nucleon
- Omega baryon
- Sigma baryon
- Timeline of particle discoveries
References
{{Reflist|25em}}External links
- REPORT
, Listings for Xi particles
, Particle Data Group
,weblink
, 2007-07-31, dead
,weblink" title="archive.today/20121212045433weblink">weblink
, 2012-12-12
, , Particle Data Group
,weblink
, 2007-07-31, dead
,weblink" title="archive.today/20121212045433weblink">weblink
, 2012-12-12
- WEB
, Direct observation of the strange b baryon Xi(b)-
, Stanford University
,weblink" title="archive.today/20121215010243weblink">weblink
, , Stanford University
,weblink" title="archive.today/20121215010243weblink">weblink
- PRESS RELEASE
,
- PRESS RELEASE
,
- WEB
, Observation and mass measurement of the baryon Xi(b)-
, Stanford University
,weblink" title="archive.today/20120526104150weblink">weblink
, {{Particles}}{{Authority control}}, Stanford University
,weblink" title="archive.today/20120526104150weblink">weblink
- content above as imported from Wikipedia
- "Xi baryon" does not exist on GetWiki (yet)
- time: 3:35pm EDT - Sat, May 04 2024
- "Xi baryon" does not exist on GetWiki (yet)
- time: 3:35pm EDT - Sat, May 04 2024
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