  In this paper we study the localization transition of Dirac eigenmodes in
quenched QCD. We determined the temperature dependence of the mobility edge in
the quark-gluon plasma phase near the deconfining critical temperature. We
calculated the critical temperature where all of the localized modes disappear
from the spectrum and compared it with the critical temperature of the
deconfining transition. We found that the localization transition happens at
the same temperature as the deconfining transition which indicates a strong
relation between the two phenomena.
