Groupoid of orientational variants

被引:87
作者
Cayron, C [1 ]
机构
[1] CEA Grenoble, DRT, LITEN, F-38054 Grenoble, France
来源
ACTA CRYSTALLOGRAPHICA SECTION A | 2006年 / 62卷
关键词
D O I
10.1107/S010876730503686X
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
Daughter crystals in orientation relationship with a parent crystal are called variants. They can be created by a structural phase transition (Landau or reconstructive), by twinning or by precipitation. Internal and external classes of transformations defined from the point groups of the parent and daughter phases and from a transformation matrix allow the orientations of the distinct variants to be determined. These are algebraically identified with left cosets and their number is given by the Lagrange formula. A simple equation links the numbers of variants of the direct and inverse transitions. The equivalence classes on the transformations between variants are isomorphic to the double cosets (operators) and their number is given by the Burnside formula. The orientational variants and the operators constitute a groupoid whose composition table acts as a crystallographic signature of the transition. A general method that determines if two daughter variants can be inherited from more than one parent crystal is also described. A computer program has been written to calculate all these properties for any structural transition; some results are given for Burgers transitions and for martensitic transitions in steels. The complexity, irreversibility and entropy of fractal systems constituted by orientational variants generated by thermal cycling are briefly discussed.
引用
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页码:21 / 40
页数:20
相关论文
共 57 条
[1]  
AKBAY B, 1994, J APPL CRYSTALLOGR, V27, P379
[2]   From knowledge, knowability and the search for objective randomness to a new vision of complexity [J].
Allegrini, P ;
Giuntoli, M ;
Grigolini, P ;
West, BJ .
CHAOS SOLITONS & FRACTALS, 2004, 20 (01) :11-32
[3]  
Bollmann W, 1982, Crystal lattices, interfaces, matrices
[4]  
Bollmann W, 1970, CRYSTAL DEFECTS CRYS
[5]  
Bradley C. J., 1972, MATH THEORY SYMMETRY
[6]  
BRANDT H, 1926, MATH ANN, V96, P360
[7]   On the process of transition of the cubic-body-centered modification into the hexagonal-close-packed modification of zirconium [J].
Burgers, WG .
PHYSICA, 1934, 1 :561-586
[8]  
Cahn J. W., 1981, SOLID SOLID PHASE TR, P3
[9]  
Cayron C., 2000, THESIS EPFL LAUSANNE
[10]  
CAYRON C, 2006, UNPUB ACTA CRYST A