Treatise on Materials Science and TechnologyHerbert Herman |
From inside the book
Results 1-3 of 38
Page 39
... planes through these centers . In principle therefore these planes are also the interfacial planes of the elastic continua . Mathematically the plane z = 0 is thus assumed to be one of these , the specific one depending on which crystal ...
... planes through these centers . In principle therefore these planes are also the interfacial planes of the elastic continua . Mathematically the plane z = 0 is thus assumed to be one of these , the specific one depending on which crystal ...
Page 76
... plane . If this crystal is straightened as in Fig . 29 ( c ) , a constant gradient of strain in the direction of z is set up resulting in a compression above and an extension below the dotted neutral plane AA ' . A close similarity with ...
... plane . If this crystal is straightened as in Fig . 29 ( c ) , a constant gradient of strain in the direction of z is set up resulting in a compression above and an extension below the dotted neutral plane AA ' . A close similarity with ...
Page 137
... plane , i.e. , the plane containing ko and k1 , is often a symmetry plane of the crystal investigated . In such cases Ŝ ( k , ) is equal to Ŝ ( −κ , ) and therefore Ŝ ( ) is an extremum with respect to κ ,. This means Ŝ changes in ...
... plane , i.e. , the plane containing ko and k1 , is often a symmetry plane of the crystal investigated . In such cases Ŝ ( k , ) is equal to Ŝ ( −κ , ) and therefore Ŝ ( ) is an extremum with respect to κ ,. This means Ŝ changes in ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
11 other sections not shown
Common terms and phrases
a-site alloy Amer anisotropy Appl approximation atoms average axis B₁ Bragg Bragg reflections c-sites calculated cations coefficients coherent compounds concentration configuration constant Cooper pairs curve Debye-Waller factor defect density dependence discussed displacement elastic electron energy epitaxial equation experimental factor ferrimagnetic field film flux lines function garnet garnet structure GdIG Geller IAEA impurity Inelastic Scattering interaction interface iron garnets k₁ lattice constant lattice parameter Lett magnetic magnetocrystalline anisotropy measured Merwe method misfit misfit dislocations mode neutron scattering normal obtained overgrowth phase phonon Phys plane potential Proc properties rare earth rare earth ions reciprocal lattice resolution sample scattering cross section shown in Fig single crystal small angle solid strain stress sublattice substrate superconducting surface symmetry Table temperature tetrahedral thermal thickness transition metal values vector X-ray YGaG