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−) multiplet and a (0+,1+) heavy spin
multiplet. Consequently the mass difference of the two multiplets is given by a
Goldberger--Treiman relation and gA is found to be small. The Isgur--Wise
function, ξ(w), the decay constant, fB, and other observables are
studied.Comment: 42 pages, SSCL-PP-243; Fermi-Pub-93/059-