Treatise on Materials Science and TechnologyHerbert Herman |
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Page 237
... density H2 / 8π . Thus we get for finite applied fields AGS = AGso + ( H22 / 8π ) Therefore , whenever ( 10 ) H1 ... density of Cooper pairs n . The field expulsion energy density [ H. - H ( x ) ] 2 / 8π is also x dependent , but varies ...
... density H2 / 8π . Thus we get for finite applied fields AGS = AGso + ( H22 / 8π ) Therefore , whenever ( 10 ) H1 ... density of Cooper pairs n . The field expulsion energy density [ H. - H ( x ) ] 2 / 8π is also x dependent , but varies ...
Page 254
... density of states near the Fermi surface is quite important . Most valuable from a macroscopic point of view are optical measurements of the electron density of state ( i.e. , photoemission and reflectivity ) . However , problems of ...
... density of states near the Fermi surface is quite important . Most valuable from a macroscopic point of view are optical measurements of the electron density of state ( i.e. , photoemission and reflectivity ) . However , problems of ...
Page 262
... density and critical current density , these two terms are used almost synonymously by some authors . C. Experimental Methods Inside a homogeneous isotropic specimen , p , will depend on the density n of flux lines only . Since n = B ...
... density and critical current density , these two terms are used almost synonymously by some authors . C. Experimental Methods Inside a homogeneous isotropic specimen , p , will depend on the density n of flux lines only . Since n = B ...
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