  The leading-order hadronic contribution to the anomalous magnetic moment of
the muon is given by a weighted integral over the subtracted hadronic vacuum
polarization. This integral is dominated by euclidean momenta of order the muon
mass which are not available on current lattice volumes with periodic boundary
conditions. Twisted boundary conditions can in principle help access momenta of
any size even in a finite volume. We investigate the implementation of twisted
boundary conditions both numerically (using all-mode averaging for improved
statistics) and analytically, and present our initial results.
