We present and contrast two distinct ways of including extremal black holes
in a Lorentzian Hamiltonian quantization of spherically symmetric Einstein
-Maxwell theory First, we formulate the classical Hamiltonian dynamics with
boundary conditions appropriate for extremal black holes only The Hamilton
ian contains no surface term at the internal infinity, for reasons related
to the vanishing of the extremal hole surface gravity, and quantization yie
lds a vanishing black hole entropy. Second, we give a Hamiltonian quantizat
ion that incorporates extremal black holes as a limiting case of nonextrema
l ones, and examine the classical limit in terms of wave packets. The sprea
ding of the packets, even the ones centered about extremal black holes, is
consistent with continuity of the entropy in the extremal limit, and thus w
ith the Bekenstein-Hawking entropy even for the extremal holes. The discuss
ion takes place throughout within Lorentz-signature spacetimes.