Components of a chiral coefficient

John F. Donoghue and Barry R. Holstein
Phys. Rev. D 46, 4076 – Published 1 November 1992
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Abstract

One of the coefficients that parametrizes the chiral Lagrangian of QCD is expressible in terms of a sum rule for which the integrand is known from experiment. We confront two model calculations of this coefficient with the behavior of the data. The model related to vector dominance reproduces the sumrule behavior very well, whereas a one-loop chiral quark model calculation fails badly. The sum rule allows one to identify those ingredients which are needed to make the quark method more realistic.

  • Received 1 June 1992

DOI:https://doi.org/10.1103/PhysRevD.46.4076

©1992 American Physical Society

Authors & Affiliations

John F. Donoghue

  • Department of Physics and Astronomy, University of Massachusetts, Amherst, Massachusetts 01003

Barry R. Holstein

  • Department of Physics and Astronomy, University of Massachusetts, Amherst, Massachusetts 01003
  • Institute for Nuclear Theory, University of Washington, Seattle, Washington 98195

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Vol. 46, Iss. 9 — 1 November 1992

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