  We discuss Wu-Yang type solutions of the Maxwell-Chern-Simons and the
Yang-Mills-Chern-Simons theories. There exists a natural scale of length which
is determined by the inverse topological mass. We obtain the non-abelian
solution by means of a SU(2) gauge transformation of Dirac magnetic monopole
type solution. In the abelian case, field strength locally determines the gauge
potential up to a closed term via self-duality equation. We introduce a
transformation of the gauge potential using dual field strength which can be
identified with the gauge transformation in the abelian solution. Then we
present Hopf map from S^3 to S^2 including the topological mass. This leads to
a reduction of the field equation onto S^2 using local sections of S^3. The
local solutions possess a composite structure consisting of both magnetic and
electric charges. These naturally lead to topologically massive Wu-Yang
solution which is based on patching up the local potentials by means of a gauge
transformation. We also discuss solutions with different first Chern numbers.
There exist a fundamental scale over which the gauge function is single-valued
and periodic for any integer in addition to the fact that it has a smaller
period. We also discuss Dirac quantization condition. We present a
stereographic view of the fibres in the Hopf map. Meanwhile Archimedes map
yields a simple geometric picture for the Wu-Yang solution. We also discuss
holonomy of the gauge potential and the dual-field on S^2. Finally we point out
a naive identification of the natural length scale introduced by the
topological mass with Hall resistivity.
