Treatise on Materials Science and TechnologyHerbert Herman |
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Page 12
... condition for insolubility , which , though sufficient , is clearly not a necessary condition . Note that temperature activated diffusion is a prerequisite for dissolution and unless the temperature is high enough the dissolution is ...
... condition for insolubility , which , though sufficient , is clearly not a necessary condition . Note that temperature activated diffusion is a prerequisite for dissolution and unless the temperature is high enough the dissolution is ...
Page 13
... condition ( 2.21 ) should not recur for the second and subsequent layers , which it would on a nearest neighbor bond hypothesis , or even go over into the condition fA < fB + ĴAB ( 2.22 ) for three - dimensional growth . Which way it ...
... condition ( 2.21 ) should not recur for the second and subsequent layers , which it would on a nearest neighbor bond hypothesis , or even go over into the condition fA < fB + ĴAB ( 2.22 ) for three - dimensional growth . Which way it ...
Page 29
... condition for the coherent con- figuration , when the misfits are equal but opposite in sign , is 0 < I / P < 1 ( 3.60 ) Analogous relationships may be written for the metastability conditions for a boundary ledge parallel to the x axis ...
... condition for the coherent con- figuration , when the misfits are equal but opposite in sign , is 0 < I / P < 1 ( 3.60 ) Analogous relationships may be written for the metastability conditions for a boundary ledge parallel to the x axis ...
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