Treatise on Materials Science and TechnologyHerbert Herman |
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Page 240
... field He1 it becomes energetically favorable to produce flux lines . In complete analogy to Eq . ( 10 ) , He1 can be expressed in terms of the free energy per length of a flux line & o ( for H2 = 0 ) and the reduction in magnetic field ...
... field He1 it becomes energetically favorable to produce flux lines . In complete analogy to Eq . ( 10 ) , He1 can be expressed in terms of the free energy per length of a flux line & o ( for H2 = 0 ) and the reduction in magnetic field ...
Page 259
... flux lines is useful for technical applications . In the following sections the basic physical mechanisms involved in flux pinning will be reviewed . A. Flux Line Lattice A single flux line has a normal core surrounded by circular ...
... flux lines is useful for technical applications . In the following sections the basic physical mechanisms involved in flux pinning will be reviewed . A. Flux Line Lattice A single flux line has a normal core surrounded by circular ...
Page 260
... flux lines is much smaller than the others near He1 ( Labusch , 1967 ) and even goes to zero when the applied field ... flux line lattice is astonishingly good even during flux flow . B. Forces on Flux Lines The flux lines do not only ...
... flux lines is much smaller than the others near He1 ( Labusch , 1967 ) and even goes to zero when the applied field ... flux line lattice is astonishingly good even during flux flow . B. Forces on Flux Lines The flux lines do not only ...
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