Treatise on Materials Science and TechnologyHerbert Herman |
From inside the book
Results 1-3 of 28
Page 109
... wave is given by a ( 0 , 0 , ko ) A ( K ) = eilkreia . P r ( II.1 ) * 1 with P = 1 for neutrons ; k 。 and k1 are the wave vectors of the incident and scattered waves , respectively . The magnitude of k is given by | k | = k = 2π / λ ...
... wave is given by a ( 0 , 0 , ko ) A ( K ) = eilkreia . P r ( II.1 ) * 1 with P = 1 for neutrons ; k 。 and k1 are the wave vectors of the incident and scattered waves , respectively . The magnitude of k is given by | k | = k = 2π / λ ...
Page 353
... waves . Particles with spin wave properties are called magnons . There is extensive literature covering the resonance linewidths in garnets ( Sparks , 1964 ; Morrish , 1965 ; von Aulock , 1965 , for example ) . The relaxation processes ...
... waves . Particles with spin wave properties are called magnons . There is extensive literature covering the resonance linewidths in garnets ( Sparks , 1964 ; Morrish , 1965 ; von Aulock , 1965 , for example ) . The relaxation processes ...
Page 372
... wave vectors of the three interacting acoustic phonons combine to equal a wave vector of the reciprocal lattice . The wave vectors of the reciprocal lattice are very small in garnets because of the large size of its unit cell . The ...
... wave vectors of the three interacting acoustic phonons combine to equal a wave vector of the reciprocal lattice . The wave vectors of the reciprocal lattice are very small in garnets because of the large size of its unit cell . 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