Treatise on Materials Science and TechnologyHerbert Herman |
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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
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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