A. Hountas et G. Tsoucaris, TWIN VARIABLES AND DETERMINANTS IN DIRECT-METHODS, Acta crystallographica. Section A, Foundations of crystallography, 51, 1995, pp. 754-763
In most algorithms of direct methods, the variables are the normalized
structure factors (SF) E(H). An alternative set of variables is propo
sed which provides more flexibility for handling, in a single algorith
m, phase relationships and direct-space constraints, as well as the co
mplete set of diffraction data. This set of variables Psi(H) consists
of SF associated with a complex periodic function psi(r) such that rho
(r) = \psi(r)\(2). The pair of variables {E(H), Psi(H)}, called twin v
ariables, play a crucial role in the subsequent theory. The phase rela
tions are enhanced by using pairs of non-negative 'twin determinants'
{D-m,D-m+1'}; D-m is a classical Karle-Hauptman (K-H) determinant invo
lving E and D'(m+1) is generated by bordering D-m with an (m+1)th row
and column containing Psi. The associated regression equation establis
hes a relation between E and Psi. Furthermore, a remarkable expression
is obtained for the gradient of the phase given by the classical tang
ent formula, as well as for the gradients involved in the related form
ulae pertaining to the Psi set. The flexibility of the algorithm is il
lustrated by the ab initio transferring to the Psi set of the a priori
known information (such as the whole set of the observed moduli), bef
ore starting the sequential phase determination of the unknown phases.
All constraints are included in a global minimization function. Analy
tical formulae are given for the gradient of this function with respec
t to the Psi set of variables. In the final result, the Psi set is sim
ultaneously compatible in the least-squares sense with the whole set o
f observed SF and with various other constraints and phase relations.
Application to two known structures permitted testing the different pa
rts of the algorithm.