Ferroelastic dynamics and strain compatibility

Physical Review B - Condensed Matter and Materials Physics

Volumn 67, Issue 2, 2003, Pages 241141-2411427

  Lookman, T ^a   Shenoy, S R ^b   Rasmussen, K O ^a   Saxena, A ^a   Bishop, A R ^a  

^a LOS ALAMOS NATIONAL LABORATORY   (United States)

^b ABDUS SALAM INTERNATIONAL CENTRE FOR THEORETICAL PHYSICS   (Italy)

Author keywords

[No Author keywords available]

Indexed keywords

ALLOY; METAL;

ACOUSTICS; ANISOTROPY; ARTICLE; CALCULATION; DENSITY; DYNAMICS; ELASTICITY; ENERGY; FORCE; FRICTION; GEOMETRY; MATHEMATICAL ANALYSIS; MOTION; NOISE; OSCILLATOR; PARAMETER; STRESS STRAIN RELATIONSHIP; TENSION; TIME;

EID: 3543069175     PISSN: 01631829     EISSN: None     Source Type: Journal    
DOI: None     Document Type: Article

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44. s(k→, M(k) will also use this compact notation (s=1,2,3). Of course, labels of points in the Brillouin zone k→, still stand for the actual wave vector k→=!k→!k̂. To emphasize that textural nonuniformity results from the large-scale compatibility properties of the ("anisotropic continuum") solid, rather than from trivial small-scale discreteness, we use the long wavelength U(k̂) in simulations.
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