Abstract

The chiral Lagrangian for Goldstone boson scattering is a power series expansion in numbers of derivatives. Each successive term is suppressed by powers of a scale, Λχ\Lambda_\chi, which must be less than of order 4πf/N4\pi f/\sqrt{N} where ff is the Goldstone boson decay constant and NN is the number of flavors. The chiral expansion therefore breaks down at or below 4πf/N4 \pi f/\sqrt{N}. We argue that the breakdown of the chiral expansion is associated with the appearance of physical states other than Goldstone bosons. Because of crossing symmetry, some ``isospin'' channels will deviate from their low energy behavior well before they approach the scale at which their low energy amplitudes would violate unitarity. We argue that the estimates of ``oblique'' corrections from technicolor obtained by scaling from QCD are untrustworthy.Comment: harvmac, 18 pages (3 figures), HUTP-92/A025, BUHEP-92-18, new version fixes a TeX problem in little mod

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    Last time updated on 03/01/2020