  In this work we present a new class of N=1 supersymmetric confining gauge
theories, with strikingly simple infrared theories that descend from intricate
interconnected networks of product gauge groups. A diagram of the gauge groups
and the charged matter content of the ultraviolet theory has the structure of a
triangular lattice, with $SU(N)$ or $SU(3 N)$ gauge groups at each of the
vertices, connected by bifundamental chiral superfields. This structure admits
a $U(1)_R$ conserving superpotential with marginal trilinear operators. With
the introduction of this superpotential, the $SU(3N)$ and $SU(N)$ gauge groups
confine: in the far infrared limit of the supersymmetric theory, the relevant
degrees of freedom are gauge invariant "mesons" and "baryons." In this paper we
show how the properties of the infrared degrees of freedom depend on the
topology and shape of the moose/quiver ``lattice'' of the original gauge
theory. We investigate various deformations of the theory, and propose some
phenomenological applications for BSM models.
