Treatise on Materials Science and TechnologyHerbert Herman |
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Page 2
... phases , A and B , say . Accordingly , a surface , being the boundary region between a gas phase and solid or liquid phase , is a special kind of interface . The interface differs in physical , chemical , and other properties , from ...
... phases , A and B , say . Accordingly , a surface , being the boundary region between a gas phase and solid or liquid phase , is a special kind of interface . The interface differs in physical , chemical , and other properties , from ...
Page 237
... phase cannot exist because it has a higher free energy than the normal phase . The same arguments can be used to ... phases . The field expulsion energy density as well as the condensation energy density are plotted schematically ...
... phase cannot exist because it has a higher free energy than the normal phase . The same arguments can be used to ... phases . The field expulsion energy density as well as the condensation energy density are plotted schematically ...
Page 313
... phases with those of the liquid or orthoferrite with which they are in equilibrium . As the yttrium concentration of the total composition is increased , the aluminum com- position in the equilibrium garnet phase is decreased . The ...
... phases with those of the liquid or orthoferrite with which they are in equilibrium . As the yttrium concentration of the total composition is increased , the aluminum com- position in the equilibrium garnet phase is decreased . The ...
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