Treatise on Materials Science and Technology, Volume 2 |
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Page 236
At absolute zero the thermodynamic critical field H . ( O ) is given by H . ( 0 ) 2 / 81
= 1 / 2N ( 0 ) 42 ( 6 ) The critical field falls off with increasing temperature
approximately as H . ( T ) / H . ( 0 ) = 1 – ( T / T . ) 2 Modifications to the BCS
theory ...
At absolute zero the thermodynamic critical field H . ( O ) is given by H . ( 0 ) 2 / 81
= 1 / 2N ( 0 ) 42 ( 6 ) The critical field falls off with increasing temperature
approximately as H . ( T ) / H . ( 0 ) = 1 – ( T / T . ) 2 Modifications to the BCS
theory ...
Page 237
field Ha , the field will penetrate into the normal metal but not into the
superconductor . To get the difference of the free energies for H , + 0 , we
therefore have to add the field expulsion energy density H , ? / 87 . Thus we get
for finite applied ...
field Ha , the field will penetrate into the normal metal but not into the
superconductor . To get the difference of the free energies for H , + 0 , we
therefore have to add the field expulsion energy density H , ? / 87 . Thus we get
for finite applied ...
Page 302
There are many significant achievements in this field and numerous books and
treatises on this subject ( Orgel , 1960 ; Griffith , 1961 ; Ballhausen , 1962 ) to
which all interested readers are referred . There have also been specific studies
on ...
There are many significant achievements in this field and numerous books and
treatises on this subject ( Orgel , 1960 ; Griffith , 1961 ; Ballhausen , 1962 ) to
which all interested readers are referred . There have also been specific studies
on ...
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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