  Two distinct phase transitions occur at different temperatures in QCD with
adjoint fermions (aQCD): deconfinement and chiral symmetry restoration. In this
model, quarks do no explicitely break the center Z(3) symmetry and therefore
the Polyakov loop is a good order parameter for the deconfinement transition.
We study monopole condensation by inspecting the expectation value of an
operator which creates a monopole. Such a quantity is expected to be an order
parameter for the deconfinement transition as in the case of fundamental
fermions.
