Treatise on Materials Science and TechnologyHerbert Herman |
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Page 36
... misfit - must eventually become unstable at large enough thick- nesses . Even though the theory is not valid for thick overgrowths , it is evident that in the new stable configuration the misfit would be partially accommodated by ...
... misfit - must eventually become unstable at large enough thick- nesses . Even though the theory is not valid for thick overgrowths , it is evident that in the new stable configuration the misfit would be partially accommodated by ...
Page 62
... misfit parameter no = 2 ( b− a ) / ( a + b ) = c / p . Curves : A , B , C , D , and F correspond respectively to t / a = 1 , 3 , 5 , 10 , and ∞ ( Ball , 1970 ) . 1.0 ENERGY 0.5 C A B 0.05 0.10 MISFIT C / p 0.15 0.20 Fig . 22. Mean misfit ...
... misfit parameter no = 2 ( b− a ) / ( a + b ) = c / p . Curves : A , B , C , D , and F correspond respectively to t / a = 1 , 3 , 5 , 10 , and ∞ ( Ball , 1970 ) . 1.0 ENERGY 0.5 C A B 0.05 0.10 MISFIT C / p 0.15 0.20 Fig . 22. Mean misfit ...
Page 73
... misfit ŋo = −eo / ( 1 + ₹ eo ) . A , B , and C for ET , min , Eн , and 2Em , respectively ( Ball , 1970 ) . D. Discussion The expressions , deduced in Section V , for the dependence of the energy , associated with misfit dislocations ...
... misfit ŋo = −eo / ( 1 + ₹ eo ) . A , B , and C for ET , min , Eн , and 2Em , respectively ( Ball , 1970 ) . D. Discussion The expressions , deduced in Section V , for the dependence of the energy , associated with misfit dislocations ...
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