Tails in the density of electron states in diluted magnetic semiconduc
tors are examined theoretically. The exchange interaction between a ch
arge carrier and magnetic ions makes the energy dependence of the dens
ity of states in the tails markedly different from those known for non
magnetic solid solutions. The cases of uncorrelated and strongly corre
lated disorder are analyzed. In both cases the density of states in th
e tail turns out to be nonmonotonic. In the case of uncorrelated disor
der the density of states has a gap, while it possesses a deep valley
in the case of strongly correlated disorder. The thermal disorder in t
he spin system of the ions makes the density of states temperature dep
endent. Some possible experimental manifestations of these features of
the tails in diluted magnetic semiconductors are discussed.