  In earlier publications we have analyzed the strong and radiative decays of
heavy hadrons in a formalism which incorporates both heavy-quark and chiral
symmetries. In particular, we have derived a heavy-hadron chiral Lagrangian
whose coupling constants are related by the heavy-quark flavor-spin symmetry
arising from the QCD Lagrangian with infinitely massive quarks. In this paper,
we re-examine the structure of the above chiral Lagrangian by including the
effects of $1/m_Q$ corrections in the heavy quark effective theory. The
relations among the coupling constants, originally derived in the heavy-quark
limit, are modified by heavy quark symmetry breaking interactions in QCD. Some
of the implications are discussed.
