Structure and thermodynamics of bulk homopolymer solid interfaces: a site lattice model approach

1988 ◽  
Vol 21 (5) ◽  
pp. 1400-1410 ◽  
Author(s):  
Doros N. Theodorou
2002 ◽  
Vol 749 ◽  
Author(s):  
B.Q. Li ◽  
Y.F. Shi ◽  
J. Bording ◽  
J.M. Zuo

ABSTRACTWe report an experimental investigation on the morphology and orientation of Ag nanoclusters by RT deposition and subsequent annealing. We show that epitaxial Ag clusters of 2 ∼ 6 nm in diameter can be synthesized in this way. The RT self-assembled Ag clusters grow as mostly single-crystal crystallites with Ag(111)//Si(111), but the in-plane orientation has a dispersion of ∼ 9° centering at Si[110] direction. Upon annealing, the Ag clusters drastically rotated to the epitaxial configuration with the in-plane orientation aligned to the Ag[110] //Si[110] direction. The rotation and epitaxy of the Ag nanoclusters are explained based on a coincident site lattice model and interface energy minimization.


1998 ◽  
Vol 108 (21) ◽  
pp. 9050-9061 ◽  
Author(s):  
Kevin Leung ◽  
Félix S. Csajka
Keyword(s):  

2019 ◽  
Vol 228 (1) ◽  
pp. 55-68 ◽  
Author(s):  
Emilio N. M. Cirillo ◽  
Matteo Colangeli ◽  
Ellen Moons ◽  
Adrian Muntean ◽  
Stela-Andrea Muntean ◽  
...  

2015 ◽  
Vol 24 (2) ◽  
pp. 028701 ◽  
Author(s):  
Zi-Cong Zhou ◽  
Fang-Ting Lin ◽  
Bo-Han Chen
Keyword(s):  

2016 ◽  
Vol 49 (6) ◽  
pp. 2031-2035 ◽  
Author(s):  
Xuefei Huang ◽  
Weigang Huang

The crystallography of the Mg2Y precipitates in an Mg–Cu–Mn–Zn–Y damping alloy has been characterized by transmission electron microscopy. The novel orientation relationship between Mg2Y and the α-Mg matrix was determined as [0001]p//[0001]α, 〈10{\overline 1}0〉p//〈2{\overline 1}{\overline 1}0〉αand 〈01{\overline 1}0〉p//〈11{\overline 2}0〉α. The precipitate exhibits a polygonal morphology with four pairs of facets, each of which is normal to a Δgvector in reciprocal space. The secondary constrained coincidence site lattice model was employed to examine the preference of each facet. The results show that a much better degree of lattice matching is realized across each facet than their vicinal orientations, indicating the energetically favoured feature of the interface. The configurations of the misfit-compensating dislocations across each interface were also calculated using the O-lattice model.


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