Treatise on Materials Science and TechnologyHerbert Herman |
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Page 11
... THERMODYNAMIC APPROACH The bicrystal is assumed to be large enough to be treated as a thermo- dynamic system . Such systems interact with the environment by the exchange of heat , work , and matter . The exchange of heat is usually ...
... THERMODYNAMIC APPROACH The bicrystal is assumed to be large enough to be treated as a thermo- dynamic system . Such systems interact with the environment by the exchange of heat , work , and matter . The exchange of heat is usually ...
Page 255
... thermodynamic properties : critical field H. 2 as a function of T. , T , as a function of pressure , and specific heat . Foner et al . ( 1972 ) have measured the critical fields at 4.2 ° K using pulsed - field techniques of Nbo.79 ( Alo ...
... thermodynamic properties : critical field H. 2 as a function of T. , T , as a function of pressure , and specific heat . Foner et al . ( 1972 ) have measured the critical fields at 4.2 ° K using pulsed - field techniques of Nbo.79 ( Alo ...
Page 259
... thermodynamic arguments ( Labusch , 1967 , 1969a ) . As in a crystal lattice , there exist dislocations in the flux line lattice that have , however , peculiar characteristics , because they are imbedded in a lattice of lines ( no jogs ...
... thermodynamic arguments ( Labusch , 1967 , 1969a ) . As in a crystal lattice , there exist dislocations in the flux line lattice that have , however , peculiar characteristics , because they are imbedded in a lattice of lines ( no jogs ...
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 R₁ 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 thermal thickness transition metal values vector X-ray YGaG νμ ΦΩ