Treatise on Materials Science and TechnologyHerbert Herman |
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Results 1-3 of 8
Page 28
... substituting from ( 3.44 ) , the result ( 1 − k ̧2 ) / kxlx + σa , ( 1 / k , l , −1 / P ) / αx < 1 / Px y y < 1 / kxlx + oα , [ ( 1 −k , 2 ) / k , l , - 1 / Px ] / x ( 3.56 ) ( 3.57 ) This reduces to σ¤ ̧1α , ( 1 , ̃ ̄ 1 28 J. H. VAN ...
... substituting from ( 3.44 ) , the result ( 1 − k ̧2 ) / kxlx + σa , ( 1 / k , l , −1 / P ) / αx < 1 / Px y y < 1 / kxlx + oα , [ ( 1 −k , 2 ) / k , l , - 1 / Px ] / x ( 3.56 ) ( 3.57 ) This reduces to σ¤ ̧1α , ( 1 , ̃ ̄ 1 28 J. H. VAN ...
Page 54
... substituting from ( 5.6 ) and ( 5.7 ) into Eq . ( 4.17 ) and putting z = 0 , one readily obtains by integration 2μ1⁄4q ( x ) = Σ [ mA „ a + 2 ( 1 −σ ) C „ a ] sin mx Ua гночь ( х ) = Σ [ mA , + 2 ( 1 - σ ) D „ o ] sin mx ( 5.8 ) where ...
... substituting from ( 5.6 ) and ( 5.7 ) into Eq . ( 4.17 ) and putting z = 0 , one readily obtains by integration 2μ1⁄4q ( x ) = Σ [ mA „ a + 2 ( 1 −σ ) C „ a ] sin mx Ua гночь ( х ) = Σ [ mA , + 2 ( 1 - σ ) D „ o ] sin mx ( 5.8 ) where ...
Page 58
... substituting ( 5.25 ) and ( 5.27 ) into ( 5.24 ) and ( ii ) by substituting ( 5.25 ) , ( 5.28 ) , ( 5.21 ) , and ( 5.27 ) into ( 5.20 ) . It follows from these identities that 2μp ( 1 + 0 ) tBn + μS / π = 0 ( 5.29 ) ( μ / d ) [ ( 2c ...
... substituting ( 5.25 ) and ( 5.27 ) into ( 5.24 ) and ( ii ) by substituting ( 5.25 ) , ( 5.28 ) , ( 5.21 ) , and ( 5.27 ) into ( 5.20 ) . It follows from these identities that 2μp ( 1 + 0 ) tBn + μS / π = 0 ( 5.29 ) ( μ / d ) [ ( 2c ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
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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