Treatise on Materials Science and TechnologyHerbert Herman |
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Page 20
... consider these briefly . On using operations of the kind ૦૬ дп = αξ δρ dp дп • = - ax sin 0 αξ dp it easily follows that Eqs . ( 3.17 ) transform into . 0 = πW , sin 2π1⁄2 - 142 { a , 2 ( 20,2 sin2 0 x - d2 + a , 2 cos20 dp2 Whe com ...
... consider these briefly . On using operations of the kind ૦૬ дп = αξ δρ dp дп • = - ax sin 0 αξ dp it easily follows that Eqs . ( 3.17 ) transform into . 0 = πW , sin 2π1⁄2 - 142 { a , 2 ( 20,2 sin2 0 x - d2 + a , 2 cos20 dp2 Whe com ...
Page 22
... consider a specific case , say 1 > 0 with б , and bx > ax · x + b . Single Dislocation . For a simple introduction to the concepts involved it is useful to consider the limiting case E1x = 0 ( kx = 1 ) ( 3.35 ) which corresponds to the ...
... consider a specific case , say 1 > 0 with б , and bx > ax · x + b . Single Dislocation . For a simple introduction to the concepts involved it is useful to consider the limiting case E1x = 0 ( kx = 1 ) ( 3.35 ) which corresponds to the ...
Page 231
... Consider Fig . 1 . Just above its superconducting transition temperature , the Nb - Ti alloy has an electrical resistivity four orders of magnitude greater than that of high purity copper . Just below its transition temperature , the ...
... Consider Fig . 1 . Just above its superconducting transition temperature , the Nb - Ti alloy has an electrical resistivity four orders of magnitude greater than that of high purity copper . Just below its transition temperature , 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