1981
DOI: 10.1103/physrevb.23.6474
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Correlation functions of amorphous multiphase systems

Abstract: We give two general integral expressions for the first and second derivatives of the so-called stick probability functions which are commonly used in analyzing x-ray-scattering results. Then it is shown that by letting the length of the stick go to zero, the limit of the second derivative can be expressed in terms of an integral over the singularity lines of the surfaces which separate the different phases of the sample. In this way one has achieved the generalization of the well-known result that the limit of… Show more

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Cited by 68 publications
(84 citation statements)
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“…We will consider now a system consisting of p homogeneous phases divided by sharp interfaces. This means that the differences of the atomic number densities can be described as [40] …”
Section: Multiphase Systemsmentioning
confidence: 99%
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“…We will consider now a system consisting of p homogeneous phases divided by sharp interfaces. This means that the differences of the atomic number densities can be described as [40] …”
Section: Multiphase Systemsmentioning
confidence: 99%
“…Small-angle scattering of three phase systems were treated first by Peterlin [38]. Multiphase systems were considered in terms of "stick probability functions" [39][40][41]. The main concern was the evaluation of the correlation function for three phase system.…”
Section: Introductionmentioning
confidence: 99%
“…The interphase surface areas obey (Goodisman & Brumberger, 1971) Sij/4 V = (dPit/dr)r = o (6) while the second derivative of Pv at r = 0 is related (Ciccariello, Cocco, Benedetti & Enzo, 1981) to the angularity of the corresponding surface. It is also useful to write (Ciccariello & Benedetti, 1985) ~(r)= E ~ijQij …”
Section: ~' Pij(r)(ni-nj) 2 V (5) Y(r) = 1 --~ Q~iq~j(n I __ Nj)2 Umentioning
confidence: 99%
“…The CLD contains the complete structural information obtainable from non-normalized SAS intensities of statistically isotropic twophase systems. The behavior of g r in the vicinity of small r is de®ned by the general structure of the interface (edges, vertices, curvature; Ciccariello et al, 1981;Ciccariello & Benedetti, 1982;Ciccariello, 1993;Sobry et al, 1994;Ciccariello & Sobry, 1995). Singularities in g and g H at ®nite values of r are related to particularities of the surface in the vicinity of minimal or maximal diameter of monodisperse particles in dilute solution (Wu & Schmidt, 1974) or of the structural unit in periodic dense two-phase systems, respectively.…”
Section: Introductionmentioning
confidence: 99%