  We present a perturbation theory for studying thermodynamic properties of the
Kondo spin liquid phase of the half-filled Kondo lattice model. The grand
partition function is derived to calculate chemical potential, spin and charge
susceptibilities and specific heat. The treatment is applicable to the model
with strong couplings in any dimensions (one, two and three dimensions). The
chemical potential equals zero at any temperatures, satisfying the requirement
of the particle-hole symmetry. Thermally activated behaviors of the
spin(charge) susceptibility due to the spin(quasiparticle) gap can be seen and
the two-peak structure of the specific heat is obtained. The same treatment to
the periodic Anderson model around atomic limit is also briefly discussed.
