  We propose a theoretical description of the sin(2 phi) current-phase relation
in SFS junctions at the 0-$\pi$ cross-over obtained in recent experiments by
Sellier et al. [Phys. Rev. Lett. 92, 257005 (2004)] where it was suggested that
a strong decoherence in the magnetic alloy can explain the magnitude of the
residual supercurrent at the 0-pi cross-over. To describe the interplay between
decoherence and elastic scattering in the ferromagnet we use an analogy with
crossed Andreev reflection in the presence of disorder. The supercurrent as a
function of the length R of the ferromagnet decays exponentially over a length
xi, larger than the elastic scattering length $l_d$ in the absence of
decoherence, and smaller than the coherence length $l_\phi$ in the absence of
elastic scattering on impurities. The best fit leads to $\xi \simeq
\xi_h^{({\rm diff})}/3$, where $\xi_h^{({\rm diff})}$ is exchange length of the
diffusive system without decoherence (also equal to $\xi$ in the absence of
decoherence). The fit of experiments works well for the amplitude of both the
sin(phi) and sin(2 phi) harmonics.
