  We present a formulation of N=(1,1), Super Yang-Mills theory in 2+1
dimensions using a transverse lattice methods that exactly preserves one
supersymmetry. First, using a Lagrangian approach we obtain a standard
transverse lattice formulation of the Hamiltonian. We then show that the
Hamiltonian also can be written discretely as the square of a supercharge and
that this produces a different result. Problems associated with the discrete
realization of the full supercharge algebra are discussed. Numerically we solve
for the bound states of the theory in the large N_c approximation and we find
good convergence. We show that the number of fermion and boson massless bound
states are closely related. Also we find that this theory admits winding states
in the transverse direction and that their masses vary inversely with the
winding number.
