Treatise on Materials Science and TechnologyHerbert Herman |
From inside the book
Results 1-3 of 31
Page 129
... limit , as used for small angle scattering , it is reasonable to use V mag = −μ „ B = − Hon yoВ where Hon = ( eh ) , ( 2mc ) , y = −1.91 , and is the Pauli operator : ☛ ( II.90 ) σ = 0 1 1 0 0 9 ) . ( 3.6-9 ) 1 0 0 i ( II.91 ) In ...
... limit , as used for small angle scattering , it is reasonable to use V mag = −μ „ B = − Hon yoВ where Hon = ( eh ) , ( 2mc ) , y = −1.91 , and is the Pauli operator : ☛ ( II.90 ) σ = 0 1 1 0 0 9 ) . ( 3.6-9 ) 1 0 0 i ( II.91 ) In ...
Page 167
... limit c1 → 0 we can interpret b1 ° [ 1 + iks1 ' ( K ) ] as a defect scattering length 6 , and with b2 = b we have N ... limit if R , ° is replaced by Ra . It seems further that in the low concentration limit and as long as no severe ...
... limit c1 → 0 we can interpret b1 ° [ 1 + iks1 ' ( K ) ] as a defect scattering length 6 , and with b2 = b we have N ... limit if R , ° is replaced by Ra . It seems further that in the low concentration limit and as long as no severe ...
Page 255
... limit . Systematic studies of V3Ga , Nb , Ga , and Ta , Ga indicate that the Pauli limit is exceeded to a greater extent for higher atomic number , indicating the importance of spin - orbit scattering . c In pressure - dependence ...
... limit . Systematic studies of V3Ga , Nb , Ga , and Ta , Ga indicate that the Pauli limit is exceeded to a greater extent for higher atomic number , indicating the importance of spin - orbit scattering . c In pressure - dependence ...
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