Treatise on Materials Science and TechnologyHerbert Herman |
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Results 1-3 of 38
Page 25
... axes T = x [ 2μt / ( 1 −σ ) ] [ ē , ( cos20 + σ sin20 ) + ē , ( sin20 + σ cos20 ) ] Txy = -2μt ( ex - ē , ) cos 0 sin デ( 3.49 ) That ē , and ē , are indeed defined by Eqs . ( 3.7 ) is most easily demonstrated by choosing the y ' axis ...
... axes T = x [ 2μt / ( 1 −σ ) ] [ ē , ( cos20 + σ sin20 ) + ē , ( sin20 + σ cos20 ) ] Txy = -2μt ( ex - ē , ) cos 0 sin デ( 3.49 ) That ē , and ē , are indeed defined by Eqs . ( 3.7 ) is most easily demonstrated by choosing the y ' axis ...
Page 339
... axis . Anisotropy energy , F1 , is required to turn M from the easy axis direction to any other direction . Phenomenologically , this magnetocrystalline anisotropy can be described , to a second approximation , for cubic crystals as FK ...
... axis . Anisotropy energy , F1 , is required to turn M from the easy axis direction to any other direction . Phenomenologically , this magnetocrystalline anisotropy can be described , to a second approximation , for cubic crystals as FK ...
Page 344
... axis which is nearly normal to the { 211 } facets . This ( 111 ) direction is the easy axis emergent from the junction of , and 19 ° 28 ' off of , the normal to the three { 211 } facets . Type II cut , as shown in Fig . 23b , is ...
... axis which is nearly normal to the { 211 } facets . This ( 111 ) direction is the easy axis emergent from the junction of , and 19 ° 28 ' off of , the normal to the three { 211 } facets . Type II cut , as shown in Fig . 23b , is ...
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 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