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The charm quark, charmed quark or c quark (from its symbol, c) is the third most massive of all quarks, a type of elementary particle. Charm quarks are found in hadrons, which are subatomic particles made of quarks. Examples of hadrons containing charm quarks include the J/ψ meson (
J/ψ
), D mesons (
D
), charmed Sigma baryons (
Σ
c
), and other charmed particles.

Charm quark
CompositionElementary particle
StatisticsFermionic
GenerationSecond
InteractionsStrong, Weak, Electromagnetic force, Gravity
Symbol
c
AntiparticleCharm antiquark (
c
)
TheorizedSheldon Glashow,
John Iliopoulos,
Luciano Maiani (1970)
DiscoveredBurton Richter et al. (SLAC)
(1974)
Samuel Ting et al. (BNL)
(1974)
Mass1.29+0.05
−0.11
 GeV/c2
[1]
Decays intoStrange quark (~95%), Down quark (~5%)[2][3]
Electric charge+2/3 e
Color chargeYes
Spin1/2
Weak isospinLH: +1/2, RH: 0
Weak hyperchargeLH: +1/3, RH: +4/3

It, along with the strange quark is part of the second generation of matter, and has an electric charge of +2/3 e and a bare mass of 1.29+0.05
−0.11
 GeV/c2
.[1] Like all quarks, the charm quark is an elementary fermion with spin 1/2, and experiences all four fundamental interactions: gravitation, electromagnetism, weak interactions, and strong interactions. The antiparticle of the charm quark is the charm antiquark (sometimes called anticharm quark or simply anticharm), which differs from it only in that some of its properties have equal magnitude but opposite sign.

The existence of a fourth quark had been speculated by a number of authors around 1964 (for instance by James Bjorken and Sheldon Glashow[4]), but its prediction is usually credited to Sheldon Glashow, John Iliopoulos and Luciano Maiani in 1970 (see GIM mechanism).[5] The first charmed particle (a particle containing a charm quark) to be discovered was the J/ψ meson. It was discovered by a team at the Stanford Linear Accelerator Center (SLAC), led by Burton Richter,[6] and one at the Brookhaven National Laboratory (BNL), led by Samuel Ting.[7]

The 1974 discovery of the
J/ψ
(and thus the charm quark) ushered in a series of breakthroughs which are collectively known as the November Revolution.

Contents

Hadrons containing charm quarksEdit

Some of the hadrons containing charm quarks include:

See alsoEdit

NotesEdit

  1. ^ a b K. Nakamura (Particle Data Group); et al. (2011). "PDGLive Particle Summary 'Quarks (u, d, s, c, b, t, b′, t′, Free)'" (PDF). Particle Data Group. Retrieved 2011-08-08.
  2. ^ R. Nave. "Transformation of Quark Flavors by the Weak Interaction". Retrieved 2010-12-06. The c quark has about 5% probability of decaying into a d quark instead of an s quark.
  3. ^ K. Nakamura et al. (Particle Data Group); et al. (2010). "Review of Particles Physics: The CKM Quark-Mixing Matrix" (PDF). Journal of Physics G. 37 (75021): 150. Bibcode:2010JPhG...37g5021N. doi:10.1088/0954-3899/37/7a/075021.
  4. ^ B.J. Bjorken, S.L. Glashow; Glashow (1964). "Elementary particles and SU(4)". Physics Letters. 11 (3): 255–257. Bibcode:1964PhL....11..255B. doi:10.1016/0031-9163(64)90433-0.
  5. ^ S.L. Glashow, J. Iliopoulos, L. Maiani; Iliopoulos; Maiani (1970). "Weak Interactions with Lepton–Hadron Symmetry". Physical Review D. 2 (7): 1285–1292. Bibcode:1970PhRvD...2.1285G. doi:10.1103/PhysRevD.2.1285.
  6. ^ J.-E. Augustin; et al. (1974). "Discovery of a Narrow Resonance in e+e Annihilation". Physical Review Letters. 33 (23): 1406. Bibcode:1974PhRvL..33.1406A. doi:10.1103/PhysRevLett.33.1406.
  7. ^ J.J. Aubert; et al. (1974). "Experimental Observation of a Heavy Particle J". Physical Review Letters. 33 (23): 1404. Bibcode:1974PhRvL..33.1404A. doi:10.1103/PhysRevLett.33.1404.

Further readingEdit