  The main focus of this work is to test the ideas related to the oblique
confinement in a theoretically controllable manner using the "deformed QCD" as
a toy model. We explicitly show that the oblique confinement in the weakly
coupled gauge theories emerges as a result of condensation of $N$ types of
monopoles shifted by the phase $\exp(i\frac{\theta+2\pi m}{N})$ in Bloch type
construction. It should be contrasted with conventional and commonly accepted
viewpoint that the confinement at $\theta\neq 0$ is due to the condensation of
the electrically charged dyons which indeed normally emerge in the systems with
$\theta\neq 0$ as a result of Witten's effect. We explain the basic reason why
the "dyon" mechanism does not materialize-- it is because the Witten's effect
holds for a static magnetic monopole treated as an external source. It should
be contrasted with our case when $N$- types of monopoles are not static, but
rather the dynamical degrees of freedom which fluctuate and themselves
determine the ground state of the system.
