Abstract

We study a solvable QCD--like toy theory, a generalization of the Nambu--Jona-Lasinio model, which implements chiral symmetries of light quarks and heavy quark symmetry. The chiral symmetric and chiral broken phases can be dynamically tuned. This implies a parity doubled heavy--light meson system, corresponding to a (0,1)(0^-,1^-) multiplet and a (0+,1+)(0^+,1^+) heavy spin multiplet. Consequently the mass difference of the two multiplets is given by a Goldberger--Treiman relation and gAg_A is found to be small. The Isgur--Wise function, ξ(w)\xi(w), the decay constant, fBf_B, and other observables are studied.Comment: 42 pages, SSCL-PP-243; Fermi-Pub-93/059-

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    Last time updated on 03/01/2020