Treatise on Materials Science and TechnologyHerbert Herman |
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Page 252
... spectrum , which is absent in the Mo spectrum , is apparent . similar to those seen in the strong - coupled nontransition metal Pb . H. G. Smith ( 1972 ) has measured the inelastic neutron scattering on NbC , TaC , HfC , and UC . Again ...
... spectrum , which is absent in the Mo spectrum , is apparent . similar to those seen in the strong - coupled nontransition metal Pb . H. G. Smith ( 1972 ) has measured the inelastic neutron scattering on NbC , TaC , HfC , and UC . Again ...
Page 253
... spectrum that enters the electron - phonon coupling parameter λ [ see Eq . ( 17 ) ] . The results for Nb3Sn are shown in Fig . 15. The zero point value of [ < w > / < w - 1 > ] 1⁄2 for Nb3Sn is found to be 178 ° K. Vieland ( 1971 ) ...
... spectrum that enters the electron - phonon coupling parameter λ [ see Eq . ( 17 ) ] . The results for Nb3Sn are shown in Fig . 15. The zero point value of [ < w > / < w - 1 > ] 1⁄2 for Nb3Sn is found to be 178 ° K. Vieland ( 1971 ) ...
Page 360
... spectrum . Similarly , the frequencies for YGaG at 393 , 340 , 257 , 234 cm1 are higher than others in the series ( Table XX ) . In the low frequency region , the 110 and 86 cm - 1 bands are missing . In the case of YIG , the 338 , 318 ...
... spectrum . Similarly , the frequencies for YGaG at 393 , 340 , 257 , 234 cm1 are higher than others in the series ( Table XX ) . In the low frequency region , the 110 and 86 cm - 1 bands are missing . In the case of YIG , the 338 , 318 ...
Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 37 |
Copyright | |
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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