Hamiltonian formulation of Wilson's lattice gauge theories

John Kogut and Leonard Susskind
Phys. Rev. D 11, 395 – Published 15 January 1975
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Abstract

Wilson's lattice gauge model is presented as a canonical Hamiltonian theory. The structure of the model is reduced to the interactions of an infinite collection of coupled rigid rotators. The gauge-invariant configuration space consists of a collection of strings with quarks at their ends. The strings are lines of non-Abelian electric flux. In the strong-coupling limit the dynamics is best described in terms of these strings. Quark confinement is a result of the inability to break a string without producing a pair.

  • Received 9 July 1974

DOI:https://doi.org/10.1103/PhysRevD.11.395

©1975 American Physical Society

Authors & Affiliations

John Kogut*

  • Laboratory of Nuclear Studies, Cornell University, Ithaca, New York 14853

Leonard Susskind

  • Belfer Graduate School of Science, Yeshiva University, New York, New York and Tel Aviv University, Ramat Aviv, Israel and Laboratory of Nuclear Studies, Cornell University, Ithaca, New York

  • *Work supported in part by the National Science Foundation.
  • Work supported in part by the National Science Foundation under Grant No. GP-38863.

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Vol. 11, Iss. 2 — 15 January 1975

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