Treatise on Materials Science and TechnologyHerbert Herman |
From inside the book
Results 1-3 of 70
Page 19
... equations 2α ̧2 2 , α , α , ( 1 + 0 ) d2n x 0 = πω , sin 2πζ - μΩ + + -σ an2 1-6 ôn ôm ax2 22¿ ' bỏ ôm ( 3.17 ) 2α , 222n ... equation in ( 3.19 ) describes an atomic configuration which represents a parallel sequence of regularly spaced ...
... equations 2α ̧2 2 , α , α , ( 1 + 0 ) d2n x 0 = πω , sin 2πζ - μΩ + + -σ an2 1-6 ôn ôm ax2 22¿ ' bỏ ôm ( 3.17 ) 2α , 222n ... equation in ( 3.19 ) describes an atomic configuration which represents a parallel sequence of regularly spaced ...
Page 21
... equations that the ŋ term vanishes , the resulting equation yields a solution for § , which , when fed into the second equation , must give a nonvanishing solution for 7. This shows that the equa- tions cannot be separated as in the ...
... equations that the ŋ term vanishes , the resulting equation yields a solution for § , which , when fed into the second equation , must give a nonvanishing solution for 7. This shows that the equa- tions cannot be separated as in the ...
Page 121
... equations above . For κa < 1 , the macroscopic equation for the self - correlation function can be used : Сself ( r , t ) = ( 4πD ) ̄3⁄41⁄2 e ̄r2 / 4Dt with SG2elf ( r , t ) dr = 1 ( II.61 ) The diffusion coefficient D is defined by ...
... equations above . For κa < 1 , the macroscopic equation for the self - correlation function can be used : Сself ( r , t ) = ( 4πD ) ̄3⁄41⁄2 e ̄r2 / 4Dt with SG2elf ( r , t ) dr = 1 ( II.61 ) The diffusion coefficient D is defined by ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
13 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 R₁ 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 thermal thickness transition metal values vector X-ray YGaG νμ ΦΩ