Rius Jordi
Institut de Ciència de Materials de Barcelona (CSIC), Campus de la UAB, 08193-Bellaterra, Catalunya, Spain.
Acta Crystallogr A. 2012 Jan;68(Pt 1):77-81. doi: 10.1107/S0108767311043145. Epub 2011 Nov 17.
The direct methods origin-free modulus sum function [Rius (1993). Acta Cryst. A49, 406-409] includes in its definition the structure factor G(Φ) of the squared crystal structure expressed in terms of Φ, the set of φ phases of the normalized structure factors E's of the crystal structure of unit-cell volume V. Here the simpler sum function variant S'(P) = ∑(H)E(-H)∫(V)δ(P,Δ)(Φ)exp(i2πHr)dV extended over all H reflections is introduced which involves no G's and in which the δ(P,Δ) function corresponds to δ(P) = FT(-1){(E(2)(H) - <E(2)>)exp[iφ(H)(Φ)]} (where FT = Fourier transform) with all values smaller than Δ = 2.5σ(P) equated to zero (σ(2)(P) is the variance of δ(P) calculable from the experimental intensities). The new phase estimates are obtained by Fourier transforming δ(P,Δ). This iterative phasing method (δ recycling) only requires calculation of Fourier transforms at two stages. Since δ(M) ≃ δ(P)/2, similar arguments are valid for δ(M) = FT(-1)[(E(H) -
直接方法中的无原点模量和函数[里乌斯(1993年)。《晶体学报》A49卷,406 - 409页]在其定义中包含了以Φ表示的平方晶体结构的结构因子G(Φ),其中Φ是单位晶胞体积为V的晶体结构的归一化结构因子E的φ相集合。这里引入了更简单的和函数变体S'(P) = ∑(H)E(-H)∫(V)δ(P,Δ)(Φ)exp(i2πHr)dV,该式扩展到所有H反射,其中不涉及G,并且δ(P,Δ)函数对应于δ(P) = FT(-1){(E(2)(H) - <E(2)>)exp[iφ(H)(Φ)]}(其中FT = 傅里叶变换),所有小于Δ = 2.5σ(P)的值都设为零(σ(2)(P)是根据实验强度可计算的δ(P)的方差)。新的相位估计值通过对δ(P,Δ)进行傅里叶变换得到。这种迭代相位方法(δ循环)只需要在两个阶段计算傅里叶变换。由于δ(M) ≃ δ(P)/2,对于δ(M) = FT(-1)[(E(H) -