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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angle anisotropy Appl approximation assumed atoms average axis c-sites calculated cations coherent concentration condition considerations constant contribution corresponding crystal curve defect density dependence determined diffusion direction discussed dislocations displacement effect elastic elastic scattering electron energy equation et al exist experimental experiments factor field flux lines follows force function garnet given gives important increasing interaction interface ions lattice length Lett limit magnetic materials measured Merwe metal method misfit mode neutron normal obtained parameter phase phonon Phys plane position potential present properties range rare earth reference region relation resolution respectively sample scattering cross section shown shows single solid solution space strain stress structure substrate superconducting surface Table temperature tetrahedral theory thermal thickness transition unit values vector X-ray