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Bottom Quark Information

The bottom quark, also known as the beauty quark, is a third-generation quark with a charge of −13 e. Although all quarks are described in a similar way by the quantum chromodynamics, the bottom quark's large bare mass (around 4,200 MeV/c2,[3] a bit more than four times the mass of a proton), combined with low values of the CKM matrix elements Vub and Vcb, gives it a distinctive signature that makes it relatively easy to identify experimentally (using a technique called B-tagging). Because three generations of quark are required for CP violation (see CKM matrix), mesons containing the bottom quark are the easiest particles to use to investigate the phenomenon; such experiments are being performed at the BaBar and Belle experiments. The bottom quark is also notable because it is a product in almost all top quark decays, and would be a frequent decay product for the hypothetical Higgs boson if it is sufficiently light.

The bottom quark was theorized in 1973 by physicists Makoto Kobayashi and Toshihide Maskawa to explain CP violation.[1] The name "bottom" was introduced in 1975 by Haim Harari.[4][5] The bottom quark discovered in 1977 by the Fermilab E288 experiment team led by Leon M. Lederman, when collisions produced bottomonium.[2][6][7] Kobayashi and Maskawa won the 2008 Nobel Prize in Physics for their explanation of CP-violation.[8][9] On its discovery, there were efforts to name the bottom quark "beauty", but "bottom" became the predominant usage.

The bottom quark can decay into either an up or charm quark via the weak interaction. Both these decays are suppressed by the CKM matrix, making lifetimes of most bottom particles (~10−12 s) somewhat higher than those of charmed particles (~10−13 s), but lower than those of strange particles (from ~10−10 to ~10−8 s).

Contents

Hadrons containing bottom quarks

Main articles: list of baryons and list of mesons

Some of the hadrons containing bottom quarks include:

See also

References

  1. ^ a b M. Kobayashi, T. Maskawa (1973). "CP-Violation in the Renormalizable Theory of Weak Interaction". Progress of Theoretical Physics 49 (2): 652–657. doi:10.1143/PTP.49.652. http://ptp.ipap.jp/link?PTP/49/652/pdf.
  2. ^ a b Fermilab (7 August 1997). "Discoveries at Fermilab - Discovery of the Bottom Quark". Press release. http://www.fnal.gov/pub/inquiring/physics/discoveries/bottom_quark_pr.html. Retrieved 2009-07-24.
  3. ^ a b c K. Nakamura et al. (Particle Data Group) (2010). "PDGLive Particle Summary 'Quarks (u, d, s, c, b, t, b', t', Free)'". Particle Data Group. http://pdg.lbl.gov/2010/tables/rpp2010-sum-quarks.pdf. Retrieved 2010-08-11.
  4. ^ H. Harari (1975). "A new quark model for hadrons". Physics Letters B 57 (3): 265. doi:10.1016/0370-2693(75)90072-6.
  5. ^ K.W. Staley (2004). The Evidence for the Top Quark. Cambridge University Press. pp. 31–33. ISBN 9780521827102. http://books.google.com/?id=K7z2oUBzB_wC.
  6. ^ L.M. Lederman (2005). "Logbook: Bottom Quark". Symmetry Magazine 2 (8). http://www.symmetrymagazine.org/cms/?pid=1000195.
  7. ^ S.W. Herb et al. (1997). "Observation of a Dimuon Resonance at 9.5 GeV in 400-GeV Proton-Nucleus Collisions". Physical Review Letters 39: 252. doi:10.1103/PhysRevLett.39.252.
  8. ^ 2008 Physics Nobel Prize lecture by Makoto Kobayashi
  9. ^ 2008 Physics Nobel Prize lecture by Toshihide Maskawa

Further reading

External links

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Noun

bottom quark (plural bottom quarks)
  1. (physics) A quark having a fractional electric charge of -1/3 and a mass about 4,100 to 4,400 MeV. Symbol: b
Synonyms
from: Wiktionary: bottom quark,
Sun Jul 10 22:23:27 2011