Treatise on Materials Science and TechnologyHerbert Herman |
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Page 259
... specimen geometry . Because of its self - energy , however , a flux line resists bending , which can give rise to transversal oscillations in the radio frequency range ( de Gennes and Matricon , 1964 ) . The triangular flux line lattice ...
... specimen geometry . Because of its self - energy , however , a flux line resists bending , which can give rise to transversal oscillations in the radio frequency range ( de Gennes and Matricon , 1964 ) . The triangular flux line lattice ...
Page 262
... specimen cross section is always equal to that measurable current passing the specimen ( Evetts et al . , 1968 ) . This is not true for the microscopic current density j = ( c / 4π ) curl h ( r ) connected with the actual fields h ( r ) ...
... specimen cross section is always equal to that measurable current passing the specimen ( Evetts et al . , 1968 ) . This is not true for the microscopic current density j = ( c / 4π ) curl h ( r ) connected with the actual fields h ( r ) ...
Page 263
... specimen must be free of flux . Kim et al . ( 1962 , 1963 ) avoided this restriction by measuring the flux through a thin superconducting tube as well as the field inside . The problem can be solved without using tubular specimens ...
... specimen must be free of flux . Kim et al . ( 1962 , 1963 ) avoided this restriction by measuring the flux through a thin superconducting tube as well as the field inside . The problem can be solved without using tubular specimens ...
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