This paper proposes a new physical method for the partial solution of the c
rystallographic phase problem by illuminating the crystal with an X-ray bea
m of limited coherence. The diffraction spots broaden and, if the coherence
length of the incident beam is small enough in all three dimensions, the d
iffraction pattern becomes continuous. Independent information about the st
ructure is then available both at the Bragg angles and at angles that do no
t satisfy the Bragg conditions. Under certain conditions, the total informa
tion is sufficient to solve the crystal structure ab initio. Two prescripti
ons for producing X-ray beams with limited coherence are given.