Treatise on Materials Science and TechnologyHerbert Herman |
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Results 1-3 of 15
Page 122
... random distribution of vacancies is assumed . Diffusion broadens the elastic scattering into a quasi- elastic line d20 = b2cy e - 2W Dy k2 do do quasiel , coh @ 2 + Dv2 2.2 ( II.66 ) where Dy is the monovacancy diffusion coefficient ...
... random distribution of vacancies is assumed . Diffusion broadens the elastic scattering into a quasi- elastic line d20 = b2cy e - 2W Dy k2 do do quasiel , coh @ 2 + Dv2 2.2 ( II.66 ) where Dy is the monovacancy diffusion coefficient ...
Page 166
... ( K ) = Nc1 ( K ) [ ( b1 ° − b2 ° ) + b ° iks1 ' ( K ) ] ( IV.44 ) ( IV.45 ) with do = ΦΩ N│c1 ( î ) | 2 | ( b1 ° −b2 ° ) + b ° iks1 ' ( k ) | 2 ( IV.46 ) coh , el , dis 1 which in case of random distribution , where | 166 W. SCHMATZ.
... ( K ) = Nc1 ( K ) [ ( b1 ° − b2 ° ) + b ° iks1 ' ( K ) ] ( IV.44 ) ( IV.45 ) with do = ΦΩ N│c1 ( î ) | 2 | ( b1 ° −b2 ° ) + b ° iks1 ' ( k ) | 2 ( IV.46 ) coh , el , dis 1 which in case of random distribution , where | 166 W. SCHMATZ.
Page 167
... random distribution , for CD < 1 and for small distortion Eq . ( 5 ) represents the defect scattering cross section if we replace R , ° by the averaged lattice vector R. Moreover , for CD < 1 it can be shown by taking into account ...
... random distribution , for CD < 1 and for small distortion Eq . ( 5 ) represents the defect scattering cross section if we replace R , ° by the averaged lattice vector R. Moreover , for CD < 1 it can be shown by taking into account ...
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