Treatise on Materials Science and TechnologyHerbert Herman |
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Page 111
... particles ( N > 1 ) is assumed to be at rest , since otherwise Doppler shift must be included . In Fig . 1 the most important quantities in the scattering MONOCHROMATOR N ATOMS ANALYZER K1 , ^ ,, Ak ,, E ,, AE , " Koo Ako EAEo Ο Fig . 1 ...
... particles ( N > 1 ) is assumed to be at rest , since otherwise Doppler shift must be included . In Fig . 1 the most important quantities in the scattering MONOCHROMATOR N ATOMS ANALYZER K1 , ^ ,, Ak ,, E ,, AE , " Koo Ako EAEo Ο Fig . 1 ...
Page 218
... particles is 2.6 R. In the case of uniform magnetization the experimental points would be on the straight line α = 1.66 . axis . The detailed study of this material by Maier ( 1969 ) has shown that in the demagnetized state the ...
... particles is 2.6 R. In the case of uniform magnetization the experimental points would be on the straight line α = 1.66 . axis . The detailed study of this material by Maier ( 1969 ) has shown that in the demagnetized state the ...
Page 353
... Particles with spin wave properties are called magnons . There is extensive literature covering the resonance linewidths in garnets ( Sparks , 1964 ; Morrish , 1965 ; von Aulock , 1965 , for example ) . The relaxation processes include ...
... Particles with spin wave properties are called magnons . There is extensive literature covering the resonance linewidths in garnets ( Sparks , 1964 ; Morrish , 1965 ; von Aulock , 1965 , for example ) . The relaxation processes include ...
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