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Chromodynamics and the quark model

  • Hadron Spectroscopy and Multiquark States
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Electron and Photon Interactions at Intermediate Energies

Part of the book series: Lecture Notes in Physics ((LNP,volume 234))

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References

  1. The idea of colour was introduced by O.W. Greenberg, Phys.Rev.Lett.13, 598 (1964). The idea that the strong interactions might be described by a non-Abelian gauge theory of colour originates in H. Fritzsch and M. Gell-Mann, Proc. XVI Int. Conf. on High Energy Physics (National Accelerator Laboratory, 1972) p.135; H. Fritzsch, M. Gell-Mann, and H. Leutwyler, Phys.Lett. 74B, 365(1973); S. Weinberg, Phys.Rev.Lett.31, 494(1973).

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  2. For reviews of lattice gauge theories and calculations, see, for example, M. Bander, Physics Reports 75, 206 (1981); J. Kogut, Rev.Mod.Phys. 55, 775(1983); L. Susskind, in Weak and Electromagnetic Interactions at High Energies, editors R. Balian and C.H. Llewellyn Smith (North Holland, Amsterdam, 1977).

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  3. See, for example, N. Isgur in Testing the Standard Model, AIP Conf. Proc., vol. 81, editors C. Heusch and W.T. Kirk (American Institute of Physics, New York, 1982), p.1.

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  4. R.L. Jaffe and K. Johnson, Phys. Lett. 60B, 201 (1976); P. Hasenfratz, R.R.Horgan, J. Kuti, and J.M. Richard, Phys.Lett. 95B, 299 (1980); T. Barnes, Z. Phys. C10, 275 (1981); T. Barnes, F.E. Close, and S. Monaghan, Nucl. Phys. B198, 380(1982); M. Chanowitz and S. Sharpe, Nucl. Phys. B222, 211(1983); E. Golowich, E. Haqq, and G. Karl, Phys. Rev. D28, 160(1983).

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  5. N. Isgur and J. Paton, Phys. Lett. 124B, 247 (1983); Phys. Rev.D (in press).

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  6. S. Godfrey, Univ. of Toronto Ph.D thesis, Dec.1983; S. Godfrey and N. Isgur, Phys. Rev.D (in press).

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  7. Hamiltonian lattice gauge theories were introduced via the SU(2) theory by J. Kogut and L. Susskind, Phys. Rev. D11, 395 (1975). See also Ref. 2.

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  8. J. Merlin and J. Paton, oxford preprint (1984).

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  9. R. Kokoski, Univ. of Toronto Ph.D. Thesis, March 1984; R. Kokoski and N. Isgur, Univ. of Toronto preprint (1984).

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  10. J. Weinstein and N. Isgur, Phys. Rev. Lett. 48, 659 (1982); Phys. Rev. D27, 588(1983). This interpretation is very close to a suggestion in the context of the bag model by R.L. Jaffe, Phys. Rev. D15, 267,281 (1977); R.L. Jaffe and K. Johnson, Phys. Lett. 60B, 201(1976); R.L. Jaffe, Phys. Rev. D17, 1444(1978).

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  11. The Mark II Collaboration, as reported by D. Hitlin in Proc. 1983 Intern. Symp. on Lepton and Photon Interactions at High Energies, eds. D.G. Cassel and D.L. Kreinick (Cornell Univ.,Ithaca, N.Y., 1983).

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  12. S. Godfrey, R. Kokoski, and N. Isgur, Phys. Lett. 141B, 439 (1984).

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  13. S. Capstick, Univ. of Toronto Ph.D. thesis,1985; S. Capstick and N. Isgur, Univ. of Toronto preprint (in preparation). It appears that the model described here will also do an excellent job in the baryon sector.

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  14. N. Isgur, R. Kokoski, and J. Paton, Univ. of Toronto preprint November 1984, predict the decay modes in which the exotic hybrid mesons of Ref. 5 should be observable.

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  15. H.J. Lipkin, private communication.

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D. Menze W. Pfeil W. J. Schwille

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© 1985 Springer-Verlag

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Isgur, N. (1985). Chromodynamics and the quark model. In: Menze, D., Pfeil, W., Schwille, W.J. (eds) Electron and Photon Interactions at Intermediate Energies. Lecture Notes in Physics, vol 234. Springer, Berlin, Heidelberg. https://doi.org/10.1007/3-540-15687-9_1

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  • DOI: https://doi.org/10.1007/3-540-15687-9_1

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