In a Hamiltonian formalism we study chiral symmetry for lattice fermio
ns formulated in terms of Shockley surface states bound to a wall in a
n extra spatial dimension. For hadronic physics this provides a natura
l scheme for taking quark masses to zero without requiring a precise t
uning of parameters. We illustrate the chiral anomaly as a flow of sta
tes in this extra dimension. We discuss two alternatives for extending
the picture to a chiral coupling of gauge fields to such fermions: on
e with a small explicit breaking of gauge symmetry and one with heavy
mirror fermions.