Treatise on Materials Science and TechnologyHerbert Herman |
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Page 117
... substitutional atom . Further , the electron distribution around a substitutional atom need not be the same as in its regular lattice . For a metal , the uncertainties above are mainly uncer- tainties in the local distribution of ...
... substitutional atom . Further , the electron distribution around a substitutional atom need not be the same as in its regular lattice . For a metal , the uncertainties above are mainly uncer- tainties in the local distribution of ...
Page 158
... substitutional atom , but also applicable for an off - center substitutional or a dumbbell interstitial atom . For a dumbbell we set for instance bb = bu ° ( eika / 2 te ika / 2 ) — bu ( IV.3 ) where a is the distance vector between the ...
... substitutional atom , but also applicable for an off - center substitutional or a dumbbell interstitial atom . For a dumbbell we set for instance bb = bu ° ( eika / 2 te ika / 2 ) — bu ( IV.3 ) where a is the distance vector between the ...
Page 159
... Substitutional disorder coupled with distortion gives correlation function Go ( r ) quite different from G °° ( r ) : νμ i . Go normally has no lattice periodicity . Nevertheless it is convenient to write Go ( r ) = [ 9,1 ( r − R ...
... Substitutional disorder coupled with distortion gives correlation function Go ( r ) quite different from G °° ( r ) : νμ i . Go normally has no lattice periodicity . Nevertheless it is convenient to write Go ( r ) = [ 9,1 ( r − R ...
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