“…The position of the fragment with respect to the symmetry elements of the space group is usually achieved by: (a) translation functions in the vector space (Braun, Hornstra & Leenhouts, 1969;Huber, 1965;Nordman & Nakatsu, 1963) or in the reciprocal space (Tollin, 1966;Crowther & Blow, 1967;Karle, 1972;Langs, 1975;Harada, Lifchitz, Berthou & Jolles, 1981); or (b) special direct-methods procedures. Among these it is worth noting: (bl) a modified tangent formula (Karle, 1968) is used to recycle in P1 phases derived from the known fragment; (b2) reflection data are expanded in the space group P1 (Doesburg & Beurskens, 1983;Bruins Slot & Beurskens, 1984) and coefficients for Fourier synthesis are obtained by direct methods on difference structure factors.…”