Treatise on Materials Science and TechnologyHerbert Herman |
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Results 1-3 of 53
Page 29
... follows that the condition for the coherent con- figuration , when the misfits are equal but opposite in sign , is 0 < I / P < 1 ( 3.60 ) Analogous relationships may be written for the metastability conditions for a boundary ledge ...
... follows that the condition for the coherent con- figuration , when the misfits are equal but opposite in sign , is 0 < I / P < 1 ( 3.60 ) Analogous relationships may be written for the metastability conditions for a boundary ledge ...
Page 59
... follows by letting μ , and λ → ∞o . It follows from Eqs . ( 5.31 ) , ( 5.33 ) , ( 5.35 ) , and ( 5.36 ) that 4. SCALE FACTOR Ma α v = i¿ = i ( y / 2 ) 1⁄2 B - 1 = 0 , @ = E = ( uc / 4n2 ) { Im [ √ ( i ) ] / − 2 / y } ( 5.37 ) ( 5.38 ) ...
... follows by letting μ , and λ → ∞o . It follows from Eqs . ( 5.31 ) , ( 5.33 ) , ( 5.35 ) , and ( 5.36 ) that 4. SCALE FACTOR Ma α v = i¿ = i ( y / 2 ) 1⁄2 B - 1 = 0 , @ = E = ( uc / 4n2 ) { Im [ √ ( i ) ] / − 2 / y } ( 5.37 ) ( 5.38 ) ...
Page 60
... follows using ( 5.45 ) , and E is the average energy per unit area . One may deduce from ( 4.3 ) that dn / df = 1 at f = 0 ( b = a ) so that wo = baElan ь at f = 0 = n ( 5.46 ) For the simple model of Section III , it follows from Eqs ...
... follows using ( 5.45 ) , and E is the average energy per unit area . One may deduce from ( 4.3 ) that dn / df = 1 at f = 0 ( b = a ) so that wo = baElan ь at f = 0 = n ( 5.46 ) For the simple model of Section III , it follows from Eqs ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
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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