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Lattice Quantum Chromodynamics

  • Chapter
Quarks, Leptons, and Beyond

Part of the book series: NATO ASI Series ((NSSB,volume 122))

Abstract

It is generally accepted that relativistic field theory is relevant in high energy physics. It is also recognized that even in QCD, which is asymptotically free (i. e., the interactions become weak at high enough energies) the scope of perturbation theory is very limited. In spite of the tremendous theoretical and experimental effort studying scaling, scaling violations, e+e−, lepton pair creation, jets and so on, the answer to the question whether and to what extent is QCD the theory of strong interactions, is very vague. At present-day energies it is difficult to disentangle perturbative and non-perturbative effects.

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  1. CERN, Geneva, Switzerland

    P. Hasenfratz

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  1. University of Munich, Munich, Federal Republic of Germany

    H. Fritzsch

  2. Max Planck Institute for Physics and Astrophysics, Munich, Federal Republic of Germany

    R. D. Peccei , H. Saller  & F. Wagner ,  & 

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Hasenfratz, P. (1985). Lattice Quantum Chromodynamics. In: Fritzsch, H., Peccei, R.D., Saller, H., Wagner, F. (eds) Quarks, Leptons, and Beyond. NATO ASI Series, vol 122. Springer, Boston, MA. https://doi.org/10.1007/978-1-4899-2254-0_3

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  • DOI: https://doi.org/10.1007/978-1-4899-2254-0_3

  • Publisher Name: Springer, Boston, MA

  • Print ISBN: 978-1-4899-2256-4

  • Online ISBN: 978-1-4899-2254-0

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