Treatise on Materials Science and TechnologyHerbert Herman |
From inside the book
Results 1-3 of 93
Page 81
... given subzone are additive as in Eq . ( A.12 ) , i.e. , En = E1n + E2n + En ( 7.26 ) and ( ii ) that the forces acting on unit length of dislocation lying parallel to the y axis are given by x g = 1Pxz ( x , z ) λ F2 = ( 1Px ' ( x , z ) ...
... given subzone are additive as in Eq . ( A.12 ) , i.e. , En = E1n + E2n + En ( 7.26 ) and ( ii ) that the forces acting on unit length of dislocation lying parallel to the y axis are given by x g = 1Pxz ( x , z ) λ F2 = ( 1Px ' ( x , z ) ...
Page 129
... given instead of the magnetic induc- tion B. Fortunately the Fourier transform of the magnetic interaction potential contains M in a simple form . In magnetostatics we have B ( r ) = H ( r ) + 4πM ( r ) , 4πM ( r ) , div B = 0 ; curl H ...
... given instead of the magnetic induc- tion B. Fortunately the Fourier transform of the magnetic interaction potential contains M in a simple form . In magnetostatics we have B ( r ) = H ( r ) + 4πM ( r ) , 4πM ( r ) , div B = 0 ; curl H ...
Page 368
... given by Eu CL ( REIG ) = ( WRC / WEu ) CL ( EuIG ) ( 51 ) where WRe and WEU are the masses of the rare earth ion and Eu ion , respectively ( Henderson et al . , 1969 ) . A list of the lattice specific heat temperature co- efficients ...
... given by Eu CL ( REIG ) = ( WRC / WEu ) CL ( EuIG ) ( 51 ) where WRe and WEU are the masses of the rare earth ion and Eu ion , respectively ( Henderson et al . , 1969 ) . A list of the lattice specific heat temperature co- efficients ...
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