1981
DOI: 10.1107/s0567739481001745
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A new formulation for the generation of coincidence site lattices (CSL's) in the cubic system

Abstract: The generation of tables of CSL's in the cubic system is presented with three parameters giving easy and rapid access to all the significant data characterizing a CSL" it is given by the rotation matrix from which the rotation axis and the rotation angle are easily determined. A method for the experimental determination of a CSL is presented, based on this new formulation.

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Cited by 43 publications
(29 citation statements)
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“…For the simple cubic lattice direct and reciprocalspace vectors are expressed by the same indices and the rotation matrix R*-= R. The analytical form of this matrix has been extensively studied by Bleris & Delavignette (1981). They have shown that the elements of the matrix are a function of the multiplicity of the CSL, 2, of the Miller indices of the rotation axis, u, v, w, and of three integer parameters m, n, a whose conditions limiting their possible values have been established.…”
Section: Cubic Systemmentioning
confidence: 99%
See 1 more Smart Citation
“…For the simple cubic lattice direct and reciprocalspace vectors are expressed by the same indices and the rotation matrix R*-= R. The analytical form of this matrix has been extensively studied by Bleris & Delavignette (1981). They have shown that the elements of the matrix are a function of the multiplicity of the CSL, 2, of the Miller indices of the rotation axis, u, v, w, and of three integer parameters m, n, a whose conditions limiting their possible values have been established.…”
Section: Cubic Systemmentioning
confidence: 99%
“…Its expression is given in equation (31a) of Bleris & Delavignette (1981). By computing the products R~=g~R, j= 1,2,...,24,…”
Section: Cubic Systemmentioning
confidence: 99%
“…Attempts at finding the general solution of this equation were made by Santoro & Mighell (1973) and by Bonnet & Cousineau (1977); and special methods were developed for two identical cubic lattices (Grimmer, 1974b;Bleris & Delavignette, 1981) and hexagonal lattices (Bonnet et al, 1981). In the following discussion, it will be assumed that a particular rational solution X 0 of this equation has been determined.…”
Section: Determination Of Coincidence Orientationsmentioning
confidence: 99%
“…Most of the work has been on CSL's of two identical three-dimensional lattices, especially cubic lattices (Ranganathan, 1966;Fortes, 1972;Grimmer, 1973;Grimmer, Bollmann & Warrington, 1974;Bleris & Delavignette, 1981) and hexagonal lattices (Fortes, 1973;Warrington, 1975;Bonnet, Cousineau & Warrington, 1981), although attention has also been given to the general case of two different three-dimensional lattices (Bucksch, 1972;Santoro & Mighell, 1973;Grimmer, 1976;Iwasaki, 1976;Bonnet & Cousineau, 1977;Fortes, 1977;Bacmann, 1979). These lattices are, of course, of special importance in solid-state physics and metallurgy, but recently attention has been given to lattices of higher dimension (e.g.…”
Section: Introductionmentioning
confidence: 99%
“…[3,4,5,6,7] and they are well understood. In particular one knows the coincidence rotations and has a handy parameterization for them, one knows the coincidence index Σ, the number of different CSLs for a given Σ, the generating functions, etc.…”
Section: Introductionmentioning
confidence: 99%