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
angle anisotropy Appl approximation assumed atoms average axis c-sites calculated cations coherent concentration condition considerations constant contribution corresponding crystal curve defect density dependence determined diffusion direction discussed dislocations displacement effect elastic elastic scattering electron energy equation et al exist experimental experiments factor field flux lines follows force function garnet given gives important increasing interaction interface ions lattice length Lett limit magnetic materials measured Merwe metal method misfit mode neutron normal obtained parameter phase phonon Phys plane position potential present properties range rare earth reference region relation resolution respectively sample scattering cross section shown shows single solid solution space strain stress structure substrate superconducting surface Table temperature tetrahedral theory thermal thickness transition unit values vector X-ray