  In this paper, we study the three-dimensional noncommutative
Maxwell-Chern-Simons theory. In the present analysis, a complete account for
the gauge field two-point function renormalizability is presented and physical
significant quantities are carefully established. The respective form factor
expressions from the gauge field self-energy are computed at one-loop order.
More importantly, an analysis of the gauge field dispersion relation, in search
of possible noncommutative anomalies and infrared finiteness, is performed for
three special cases, with particular interest in the highly noncommutative
limit.
