In Quark Nuclear Physics (QNP), where hadrons and nuclei are described
in terms of quarks and gluons, confinement and chiral symmetry breaki
ng are the most fundamental phenomena. The dual Ginzburg-Landau (DGL)
theory, which contains monopole fields as the most essential degrees o
f freedom and their condensation in the vacuum, is able to describe bo
th phenomena. We discuss also the recovery of the chiral symmetry and
the deconfinement phase transition at finite temperature in the DGL th
eory. As for the connection to QCD, we study the instanton configurati
ons in the abelian gauge a la 't Hooft. We find a close connection bet
ween instantons and QCD monopoles. We demonstrate also the signature o
f confinement as the appearance of long monopole trajectories in the M
A gauge for the case of dense instanton configurations.