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Down quark

From Wikipedia, the free encyclopedia
(Redirected fromDown antiquark)
Type of quark
Down quark
Compositionelementary particle
Statisticsfermionic
Familyquark
Generationfirst
Interactionsstrong,weak,electromagnetic,gravity
Symbold
Antiparticledown antiquark (d)
TheorizedMurray Gell-Mann (1964)
George Zweig (1964)
DiscoveredSLAC (1968)
Mass4.7+0.5
−0.3
 MeV/c2
[1]
Decays intostable orup quark +electron +electron antineutrino
Electric charge1/3e
Color chargeYes
Spin1/2 ħ
Weak isospinLH: −1/2,RH: 0
Weak hyperchargeLH: +1/3,RH: −2/3

Thedown quark (symbol: d) is a type ofelementary particle, and a major constituent ofmatter. The down quark is the second-lightest of allquarks, and combines with other quarks to formcomposite particles calledhadrons. Down quarks are most commonly found inatomic nuclei, where it combines withup quarks to formprotons andneutrons. The proton is made of one down quark with two up quarks, and the neutron is made up of two down quarks with one up quark. Because they are found in every single known atom, down quarks are present in all everyday matter that we interact with.

The down quark is part of thefirst generation of matter, has anelectric charge of −1/3 e and abare mass of4.7+0.5
−0.3
 MeV/c2
.[1] Like all quarks, the down quark is an elementaryfermion withspin1/2, and experiences all fourfundamental interactions:gravitation,electromagnetism,weak interactions, andstrong interactions. Theantiparticle of the down quark is thedown antiquark (sometimes calledantidown quark or simplyantidown), which differs from it only in that some of its properties haveequal magnitude but opposite sign.

Its existence (along with that of the up andstrange quarks) was postulated in 1964 byMurray Gell-Mann andGeorge Zweig to explain theEightfold Way classification scheme ofhadrons. The down quark was first observed by experiments at theStanford Linear Accelerator Center in 1968.

History

[edit]
Murray Gell-Mann
George Zweig

In the beginnings of particle physics (first half of the 20th century),hadrons such asprotons,neutrons, andpions were thought to beelementary particles. However, as new hadrons were discovered, the 'particle zoo' grew from a few particles in the early 1930s and 1940s to several dozens of them in the 1950s. The relationships between each of them was unclear until 1961, whenMurray Gell-Mann[2] andYuval Ne'eman[3] (independently of each other) proposed a hadron classification scheme called theEightfold Way, or in more technical terms,SU(3)flavor symmetry.

This classification scheme organized the hadrons intoisospin multiplets, but the physical basis behind it was still unclear. In 1964, Gell-Mann[4] andGeorge Zweig[5][6] (independently of each other) proposed thequark model, then consisting only ofup, down, andstrange quarks.[7] However, while the quark model explained the Eightfold Way, no direct evidence of the existence of quarks was found until 1968 at theStanford Linear Accelerator Center.[8][9]Deep inelastic scattering experiments indicated that protons had substructure, and that protons made of three more-fundamental particles explained the data (thus confirming the quark model).[10]

At first people were reluctant to identify the three-bodies as quarks, instead preferringRichard Feynman'sparton description,[11][12][13] but over time the quark theory became accepted (seeNovember Revolution).[14]

Mass

[edit]

Despite being extremely common, thebare mass of the down quark is not well determined, but probably lies between4.5 and 5.3 MeV/c2.[15]Lattice QCD calculations give a more precise value:4.79±0.16 MeV/c2.[16]

When found inmesons (particles made of one quark and oneantiquark) orbaryons (particles made of three quarks), the 'effective mass' (or 'dressed' mass) of quarksbecomes greater because of thebinding energy caused by thegluon field between quarks (seemass–energy equivalence). For example, the effective mass of down quarks in a proton is around300 MeV/c2. Because the bare mass of down quarks is so small, it cannot be straightforwardly calculated because relativistic effects have to be taken into account.

References

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  1. ^abM. Tanabashi et al. (Particle Data Group) (2018)."Review of Particle Physics".Physical Review D.98 (3):1–708.Bibcode:2018PhRvD..98c0001T.doi:10.1103/PhysRevD.98.030001.hdl:10044/1/68623.PMID 10020536.
  2. ^M. Gell-Mann (2000) [1964]. "The Eightfold Way: A theory of strong interaction symmetry". In M. Gell-Mann, Y. Ne'eman (ed.).The Eightfold Way.Westview Press. p. 11.ISBN 978-0-7382-0299-0.
    Original:M. Gell-Mann (1961). "The Eightfold Way: A theory of strong interaction symmetry".Synchrotron Laboratory Report CTSL-20.California Institute of Technology.
  3. ^Y. Ne'eman (2000) [1964]. "Derivation of strong interactions from gauge invariance". In M. Gell-Mann, Y. Ne'eman (ed.).The Eightfold Way.Westview Press.ISBN 978-0-7382-0299-0.
    OriginalY. Ne'eman (1961). "Derivation of strong interactions from gauge invariance".Nuclear Physics.26 (2):222–229.Bibcode:1961NucPh..26..222N.doi:10.1016/0029-5582(61)90134-1.
  4. ^M. Gell-Mann (1964). "A Schematic Model of Baryons and Mesons".Physics Letters.8 (3):214–215.Bibcode:1964PhL.....8..214G.doi:10.1016/S0031-9163(64)92001-3.
  5. ^G. Zweig (1964). "An SU(3) Model for Strong Interaction Symmetry and its Breaking".CERN Report No.8181/Th 8419.
  6. ^G. Zweig (1964). "An SU(3) Model for Strong Interaction Symmetry and its Breaking: II".CERN Report No.8419/Th 8412.
  7. ^B. Carithers, P. Grannis (1995)."Discovery of the Top Quark"(PDF).Beam Line.25 (3):4–16. Retrieved2008-09-23.
  8. ^E. D. Bloom; et al. (1969)."High-Energy Inelasticep Scattering at 6° and 10°".Physical Review Letters.23 (16):930–934.Bibcode:1969PhRvL..23..930B.doi:10.1103/PhysRevLett.23.930.
  9. ^M. Breidenbach; et al. (1969)."Observed Behavior of Highly Inelastic Electron–Proton Scattering"(PDF).Physical Review Letters.23 (16):935–939.Bibcode:1969PhRvL..23..935B.doi:10.1103/PhysRevLett.23.935.OSTI 1444731.S2CID 2575595.
  10. ^J. I. Friedman."The Road to the Nobel Prize".Hue University. Archived fromthe original on 2008-12-25. Retrieved2008-09-29.
  11. ^R. P. Feynman (1969)."Very High-Energy Collisions of Hadrons"(PDF).Physical Review Letters.23 (24):1415–1417.Bibcode:1969PhRvL..23.1415F.doi:10.1103/PhysRevLett.23.1415.
  12. ^S. Kretzer; H. Lai; F. Olness; W. Tung (2004). "CTEQ6 Parton Distributions with Heavy Quark Mass Effects".Physical Review D.69 (11) 114005.arXiv:hep-ph/0307022.Bibcode:2004PhRvD..69k4005K.doi:10.1103/PhysRevD.69.114005.S2CID 119379329.
  13. ^D. J. Griffiths (1987).Introduction to Elementary Particles.John Wiley & Sons. p. 42.ISBN 978-0-471-60386-3.
  14. ^M. E. Peskin, D. V. Schroeder (1995).An introduction to quantum field theory.Addison–Wesley. p. 556.ISBN 978-0-201-50397-5.
  15. ^J. Beringer; et al. (Particle Data Group) (2013)."PDGLive Particle Summary 'Quarks (u, d, s, c, b, t, b′, t′, Free)'"(PDF).Particle Data Group. Retrieved2013-07-23.
  16. ^Cho, Adrian (April 2010)."Mass of the Common Quark Finally Nailed Down". Science Magazine. Archived fromthe original on 2012-03-06.

Further reading

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Elementary
Fermions
Quarks
Leptons
Bosons
Gauge
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Ghost fields
Hypothetical
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Composite
Hadrons
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Exotic hadrons
Others
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