  The Periodic Anderson Model (PAM) is widely studied to understand strong
correlation physics and especially the competition of antiferromagnetism and
singlet formation. Quantum Monte Carlo (QMC) studies have focused both on
issues such as the nature of screening and locating the quantum critical point
(QCP) at zero temperature and also on possible experimental connections to
phenomena ranging from the Cerium volume collapse to the relation of the
magnetic susceptibility and Knight shift in heavy fermions. In this paper we
extend QMC work to lattices in which the conduction electron sites can have
variable coordination. This situation is relevant both to recently discovered
magnetic quasicrystals and also to magnetism in doped heavy fermion systems.
