Bottom quark

Generations of matter
Type First Second Third
Quarks
up-type up charm top
down-type down strange bottom
Leptons
charged electron muon tau
neutral electron neutrino muon neutrino tau neutrino

Bottom quark
Composition Elementary particle
Statistics Fermionic
Generation Third
Interactions Strong, Weak, Electromagnetic force, Gravity
Symbol
b
Antiparticle Bottom antiquark (
b
)
Theorized Makoto Kobayashi and Toshihide Maskawa (1973)[1]
Discovered Leon M. Lederman et al. (1977)[2]
Mass

4.18+0.03
−0.03 GeV/c2 (MS scheme)[3]

4.65+0.03
−0.03 GeV/c2 (1S scheme)[3]
Decays into

Charm quark, or

up quark
Electric charge −1/3 e
Color charge Yes
Spin 1/2
Weak isospin LH: −1/2, RH: 0
Weak hypercharge LH: 1/3, RH: −2/3

The bottom quark or b quark, also known as the beauty quark, is a third-generation quark with a charge of −1/3 e.

All quarks are described in a similar way by electroweak and quantum chromodynamics, but the bottom quark has exceptionally low rates of transition to lower-mass quarks. The bottom quark is also notable because it is a product in almost all top quark decays, and is a frequent decay product for the Higgs boson.

Name and history

The bottom quark was first described theoretically 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 was 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, by analogy of "top" and "bottom" to "up" and "down".

Distinct character

The bottom quark's "bare" mass is around 4.2 GeV/c2[3] – a bit more than four times the mass of a proton, and many orders of magnitude larger than common "light" quarks.

Although it almost-exclusively transitions from or to a top quark, the bottom quark can decay into either an up quark or charm quark via the weak interaction. CKM matrix elements Vub and Vcb specify the rates, where both these decays are suppressed, 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).[10]

The combination of high mass and low transition-rate gives experimental collision byproducts containing a bottom quark a distinctive signature that makes them relatively easy to identify using a technique called "B-tagging". For that reason, mesons containing the bottom quark are exceptionally long-lived for their mass, and are the easiest particles to use to investigate CP violation. Such experiments are being performed at the BaBar, Belle and LHCb experiments.

Hadrons containing bottom quarks

Some of the hadrons containing bottom quarks include:

See also

References

  1. 1 2 M. Kobayashi; T. Maskawa (1973). "CP-Violation in the Renormalizable Theory of Weak Interaction". Progress of Theoretical Physics. 49 (2): 652–657. Bibcode:1973PThPh..49..652K. doi:10.1143/PTP.49.652.
  2. 1 2 "Discoveries at Fermilab – Discovery of the Bottom Quark" (Press release). Fermilab. 7 August 1977. Retrieved 2009-07-24.
  3. 1 2 3 J. Beringer (Particle Data Group); et al. (2012). "PDGLive Particle Summary 'Quarks (u, d, s, c, b, t, b′, t′, Free)'" (PDF). Particle Data Group. Retrieved 2012-12-18.
  4. ↑ H. Harari (1975). "A new quark model for hadrons". Physics Letters B. 57 (3): 265. Bibcode:1975PhLB...57..265H. 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 978-0-521-82710-2.
  6. ↑ L.M. Lederman (2005). "Logbook: Bottom Quark". Symmetry Magazine. 2 (8). Archived from the original on 4 October 2006.
  7. ↑ S.W. Herb; Hom, D.; Lederman, L.; Sens, J.; Snyder, H.; Yoh, J.; Appel, J.; Brown, B.; Brown, C.; Innes, W.; Ueno, K.; Yamanouchi, T.; Ito, A.; Jöstlein, H.; Kaplan, D.; Kephart, R.; et al. (1977). "Observation of a Dimuon Resonance at 9.5 GeV in 400-GeV Proton-Nucleus Collisions". Physical Review Letters. 39 (5): 252. Bibcode:1977PhRvL..39..252H. doi:10.1103/PhysRevLett.39.252.
  8. ↑ 2008 Physics Nobel Prize lecture by Makoto Kobayashi
  9. ↑ 2008 Physics Nobel Prize lecture by Toshihide Maskawa
  10. ↑ Nave, C. R. "Transformation of Quark Flavors by the Weak Interaction". HyperPhylsics.

Further reading

This article is issued from Wikipedia. The text is licensed under Creative Commons - Attribution - Sharealike. Additional terms may apply for the media files.