2006
DOI: 10.1016/j.actamat.2005.11.021
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Domain growth and off-phase boundary structures in L12-type ordering

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Cited by 12 publications
(7 citation statements)
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“…8(b)), the boundary plane lies planes D and A. Consequently, every S ary has 12 Cu atoms as the nearest neig the same as that of the perfect D019 latt tion, for APBs of type 2 (Fig. 8(c)), the between the (01 1 0) planes A and B, thus boundary has two Sn atoms and ten Cu On the basis of the analogy between g and an elastic energy [7], the condition for isotropic media is obtained as follows;…”
Section: Resultsmentioning
confidence: 97%
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“…8(b)), the boundary plane lies planes D and A. Consequently, every S ary has 12 Cu atoms as the nearest neig the same as that of the perfect D019 latt tion, for APBs of type 2 (Fig. 8(c)), the between the (01 1 0) planes A and B, thus boundary has two Sn atoms and ten Cu On the basis of the analogy between g and an elastic energy [7], the condition for isotropic media is obtained as follows;…”
Section: Resultsmentioning
confidence: 97%
“…We derived a TDGL formulation for D0 19 type ordering in the way similar to the case of L1 2 [7]. The order parameters are well defined, and mappings obtained from simulations of TDGL equations can be compared with dark-field TEM images.…”
Section: Discussionmentioning
confidence: 99%
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“…To favor the mobility of the implanted nitrogen atoms and repair possible damage to the surface, we follow the sputtering by an annealing process, leading to the formation of a c(2x2)N reconstruction on the Cu 3 Au(100) surface, similar to that reported for Cu(100) [2]. A Cu 3 Au crystal can be in two distinct phases: an ordered L1 2 phase [16,17] upon annealing below a critical temperature T c = 663 K [18,19,20], and a disordered phase above this temperature [21,22]. While both phases have the FCC crystal structure, in the L1 2 phase the Au atoms are periodically distributed over the crystal whereas in the disordered phase they are not.…”
Section: Methodsmentioning
confidence: 94%
“…Since its observation on 1934 2) in Cu-Zn alloys (brass), this transition which is expressed by the existence of one state in which atoms are ordered in crystal lattice, has been widely studied. [3][4][5][6][7] On the basis of X-ray diffraction, it has been noticed that below certain transition temperature, the atoms can be ordered on two sublattices which interpenetrate, i.e. the atoms of every type have tendency to take specific places in the crystal lattice by changing their position.…”
Section: Introductionmentioning
confidence: 99%