Treatise on Materials Science and TechnologyHerbert Herman |
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Results 1-3 of 36
Page 107
... possible by the theoretical work of Krivoglaz ( 1969 ) , who combined electronic properties , via binding forces and the theory of thermodynamic statistics , with scattering theory in a way which allowed even an experimental physicist ...
... possible by the theoretical work of Krivoglaz ( 1969 ) , who combined electronic properties , via binding forces and the theory of thermodynamic statistics , with scattering theory in a way which allowed even an experimental physicist ...
Page 117
... possible influences have been neglected . In general , a , ( K ) is the Fourier transform of the electron distribution attached to the nuclei of atom 1 , whose position vector is r1 = R1 + u ,. In Eqs . ( 36 ) and ( 37 ) we have ...
... possible influences have been neglected . In general , a , ( K ) is the Fourier transform of the electron distribution attached to the nuclei of atom 1 , whose position vector is r1 = R1 + u ,. In Eqs . ( 36 ) and ( 37 ) we have ...
Page 119
... possible and useful . Having introduced the correlation functions , further remarks concerning X - ray scattering are possible . Because energy resolution is not possible with X - rays , the integral scattering cross section is measured ...
... possible and useful . Having introduced the correlation functions , further remarks concerning X - ray scattering are possible . Because energy resolution is not possible with X - rays , the integral scattering cross section is measured ...
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