A Planar Diagram Theory for Strong Interactions
Gerard 't Hooft (CERN)

Dec 1973 - 13 pages

  • Nucl.Phys. B72 (1974) 461
    In *Taylor, J.C. (ed.): Gauge theories in the twentieth century* 337-349
  • (1974)
  • DOI: 10.1016/0550-3213(74)90154-0
  • CERN-TH-1786

Abstract (Elsevier)
A gauge theory with colour gauge group U( N ) and quarks having a colour index running from one to N is considered in the limit N → ∞, g 2 N fixed. It is shown that only planar diagrams with the quarks at the edges dominate; the topological structure of the perturbation series in 1/ N is identical to that of the dual models, such that the number 1/ N corresponds to the dual coupling constant. For hadrons N is probably equal to three. A mathematical framework is proposed to link these concepts of planar diagrams with the functional integrals of Gervais, Sakita and Mandelstam for the dual string.


Keyword(s): INSPIRE: strong interaction | gauge field theory: U(N) | Feynman graph: planar | expansion 1/N | string model | Hamiltonian formalism
 Record added 1973-12-01, last modified 2018-03-27