  Specific features of the equilibrium current-carrying state of a Josephson
tunnel junction between diffusive superconductors are studied theoretically in
the 1D geometry. It is found that the Josephson current induces localized
states of electron excitations in the vicinity of the tunnel barrier, which are
a continuous analog of Andreev levels in a ballistic junction. The depth of the
corresponding ``potential well'' is much greater than the separation between an
Andreev level and the continuous energy spectrum boundary for the same
transmissivity of the barrier. In contrast to a ballistic junction in which the
Josephson current is transported completely by localized excitations, the
contribution to current in a diffusive junction comes from whole spectral
region near the energy gap boundary, where the density of states differs
considerably from its unperturbed value. The correction to the Josephson
current in the second order of the barrier transmissivity, which contains the
second harmonic of the phase jump, is calculated and it is found that the true
expansion parameter of the perturbation theory for a diffusive junction is not
the tunneling probability $\Gamma$ itself, but a much larger parameter $W =
(3\xi_0/4l)\Gamma$.
