  A Hamiltonian approach to black hole entropy is used to study Riemannian
Kerr-AdS solutions in the general, parity-violating Poincar\'e gauge theory.
Entropy and the asymptotic charges are entirely determined by the parity-even
sector of the theory, whereas the parity-odd contributions vanish. Entropy is
found to be proportional to the horizon area, and the first law of black hole
thermodynamics is confirmed.
