Unlike usual lattice gauge theories the use of a non–Abelian group here as spacetime
corresponds to a background Riemannian curvature. In this background we solve spin 0, 1 2
and spin 1 equations of motion, including the spin 1 or 'photon'case in the presence of
sources, ie a theory of classical electromagnetism. Moreover, we solve the U (1) Yang–Mills
theory (this differs from the U (1) Maxwell theory in noncommutative geometry), including the …