Chiral-symmetry breaking in asymptotically free theories with slowly running couplings is analyzed. When the confinement scale {Λ} is much less than the cutoff M beyond which the theory cannot be used in isolation, the dynamical mass {Σ}(p) starts from a value {}{Λ} for momenta p{}{Λ} and falls slowly for a significant range p>{Λ}. It then takes on the asymptotic form (lnp)ᵃ/p² where a>1. This behavior leads to an enhancement of the fermion condensate defined with the ultraviolet cutoff M, while the Goldstone-boson decay constant F remains essentially unaltered. In technicolor theories, with four-fermion interactions of strength {}1/M² that explicitly break some chiral symmetries, the technifermion condensate determines the values of fermion masses and pseudo-Goldstone-boson masses while F determines W and Z masses. An enhancement of the technifermion condensate will then generate fermion and pseudo-Goldstone-boson masses for higher values of M than naively expected, keeping W and Z masses nearly fixed. This could allow for an adequate suppression of the flavor-changing neutral currents that have plagued technicolor theories. Explicit gauge theories that exhibit slow running are tabulated and the results of a numerical study are reported.
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Appelquist et al. (1987) studied this question.
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