Treatise on Materials Science and TechnologyHerbert Herman |
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Page 59
... complex arguments and z2 + B - 1z + y / 2 = ( z + w + v ) ( z + w - v ) ( 5.34 ) If v is imaginary , i.e. , v = it = i ( y / 2 - B − 2 / 4 ) 1⁄2 ( 5.35 ) E = ( μc / 4n2 ) [ Im { √ ( w + i§ ) } / ¿ − 2 / y ] ( 5.36 ) where Im ...
... complex arguments and z2 + B - 1z + y / 2 = ( z + w + v ) ( z + w - v ) ( 5.34 ) If v is imaginary , i.e. , v = it = i ( y / 2 - B − 2 / 4 ) 1⁄2 ( 5.35 ) E = ( μc / 4n2 ) [ Im { √ ( w + i§ ) } / ¿ − 2 / y ] ( 5.36 ) where Im ...
Page 184
... complex field . 1. SINGLE LIGHT IMPURITY The impurity mass MD is assumed to be considerably smaller than the host atom mass Mн and the force constants remain unchanged . A localized mode with frequency w1 is given by H 2 ( g ( w ) dw ...
... complex field . 1. SINGLE LIGHT IMPURITY The impurity mass MD is assumed to be considerably smaller than the host atom mass Mн and the force constants remain unchanged . A localized mode with frequency w1 is given by H 2 ( g ( w ) dw ...
Page 192
... complex . Especially the crossing of phonon branches and mixed second - order and first - order transition causes additional complexity . A large number of investigations have been performed within the last five years at the Brookhaven ...
... complex . Especially the crossing of phonon branches and mixed second - order and first - order transition causes additional complexity . A large number of investigations have been performed within the last five years at the Brookhaven ...
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