History, quark model and the SU(3)-symmetry

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Bjorken scaling Structure-Function F2 as function of the Bjorken Variable x here called ξ for different Q² values. 2 x : = Q 2Mν is the additive term from the invariant mass Simela Aslanidou 14.12.2006
Quarks Existence of Quarks there is empirical evidence since the momentum transfer realised at SLAC was much larger than the nucleon-mass Q²>>M² this result is interpreted at the following way: the nucleon must have a substructure of quasi-free, point-like particles. Simela Aslanidou 14.12.2006
Page 1 and 2: QCD History, quark model and the SU
Page 3 and 4: History • up to the beginning of
Page 5 and 6: History • 1950´s Robert Hofstadt
Page 7 and 8: History • both, Gell-Mann and Zwe
Page 9 and 10: History • the method of the exper
Page 11 and 12: Concepts The proton is an extended
Page 13 and 14: Concepts invariant mass W² c² = P
Page 15 and 16: Inelastic scattering Displaying the
Page 17: Inelastic scattering d² σ dΩdE
Page 21 and 22: Quark model Problems • non-observ
Page 23 and 24: Necessity of the colour Quarks are
Page 25 and 26: Colour • in 1965 O.W.Greenberg in
Page 27 and 28: Colour The additive colour model Si
Page 29 and 30: Quark model • why are there three
Page 31 and 32: Simela Aslanidou 14.12.2006 Quark m
Page 33 and 34: Ratio of the cross section Comparis
Page 35 and 36: Gluons • gluons are the gauge bos
Page 37 and 38: SU(N) • group of the non-abelian
Page 39 and 40: SU(3) Why SU(3)-flavour? With the S
Page 41 and 42: The Baryon-Oktet Start from the fun
Page 43 and 44: References T. Muta, World Scientif

History, quark model and the SU(3)-symmetry

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