Treatise on Materials Science and TechnologyHerbert Herman |
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Page 254
... heat measurements ( Vieland and Wickland , 1966 , 1968 , 1969 ) , therefore , do not yield unambiguous results for the electronic specific heat coefficient y . Anomalous linear terms in the specific heat are found at temperatures where ...
... heat measurements ( Vieland and Wickland , 1966 , 1968 , 1969 ) , therefore , do not yield unambiguous results for the electronic specific heat coefficient y . Anomalous linear terms in the specific heat are found at temperatures where ...
Page 368
... heat , C1 , follows the well - known T3 law at low temperatures where the ratio 0 / T may be taken to be infinite ... heat temperature co- efficients , AL , for several ReIG and YIG is given in Table XXVII . TABLE XXVII SPECIFIC HEAT ...
... heat , C1 , follows the well - known T3 law at low temperatures where the ratio 0 / T may be taken to be infinite ... heat temperature co- efficients , AL , for several ReIG and YIG is given in Table XXVII . TABLE XXVII SPECIFIC HEAT ...
Page 370
... heat ( Henderson et al . , 1969 ) . In EuIG , the nuclear specific heat , CN , must be included . The linear residual part had a temperature coefficient of ( 0.23 ± 0.03 ) × 10-3R , and it is ~ 15 % of C , above 2 ° K , but becomes ...
... heat ( Henderson et al . , 1969 ) . In EuIG , the nuclear specific heat , CN , must be included . The linear residual part had a temperature coefficient of ( 0.23 ± 0.03 ) × 10-3R , and it is ~ 15 % of C , above 2 ° K , but becomes ...
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