We present a bond-operator mean-field theory for the Kondo lattice model at
half filling in two and three dimensions (3D). A continuous quantum phase
transition from an antiferromagnetic to a spin-gapped singlet ground state
is found at J/t = 1.505 (1.833) in 2D (3D). Additionally we evaluate the qu
asiparticle dispersions as well as the staggered magnetic moment and provid
e a comparison with complementary numerical approaches.