Treatise on Materials Science and Technology, Volume 2 |
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Page 53
The results may be useful for a two - fold layer but are inadequate for thicker ones
, because they do not allow for the proper elastic relaxation in substrate and film .
The model of Ball ( 1970 ) , described in Section V , C , is an improvement on ...
The results may be useful for a two - fold layer but are inadequate for thicker ones
, because they do not allow for the proper elastic relaxation in substrate and film .
The model of Ball ( 1970 ) , described in Section V , C , is an improvement on ...
Page 257
Since relaxation can only T 1 / T , ( sec ' ) III 야 2 0 4 0 0 1 / T ( °K ) Fig . 17 .
Logarithm of the nuclear spin - lattice relaxation rate vs . reciprocal temperature
below the superconducting transition temperature in V3 Ga1 - Snc alloys ( from
Zamir ...
Since relaxation can only T 1 / T , ( sec ' ) III 야 2 0 4 0 0 1 / T ( °K ) Fig . 17 .
Logarithm of the nuclear spin - lattice relaxation rate vs . reciprocal temperature
below the superconducting transition temperature in V3 Ga1 - Snc alloys ( from
Zamir ...
Page 353
the crystal lattice and the relaxation of magnons via various processes . It is also
a property which can be explained by quantum mechanical spin waves . Particles
with spin wave properties are called magnons . There is extensive literature ...
the crystal lattice and the relaxation of magnons via various processes . It is also
a property which can be explained by quantum mechanical spin waves . Particles
with spin wave properties are called magnons . There is extensive literature ...
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Contents
Epitaxial Interfaces | 3 |
Thin Films | 15 |
Semiinfinite Overgrowths | 52 |
Copyright | |
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angle anisotropy approximation assumed atoms average axis c-site calculated cations coherent compounds concentration condition considerations constants contribution corresponding crystal curve decreases defect density dependence determined diffusion direction discussed dislocations displacement effect elastic elastic scattering electron energy equation et al experimental experiments factor field flux flux lines follows force function garnets given gives important impurity increases interaction interface ions lattice limit magnetic materials measured Merwe metal method misfit mode neutron normal observed obtained optical parameter phase phonon Phys plane position potential present processes properties range reference region 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 wave X-ray