Treatise on Materials Science and Technology, Volume 2 |
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Page 87
18 ) Strictly speaking one should refer to the average energy per bond because
Nm is really the number of bonds in a row of Nm + 1 atoms . The dependence of
£m on Nm and Nmll is illustrated in Fig . 31 for the case defined by 1 = 7 , 1 / P =
0 ...
18 ) Strictly speaking one should refer to the average energy per bond because
Nm is really the number of bonds in a row of Nm + 1 atoms . The dependence of
£m on Nm and Nmll is illustrated in Fig . 31 for the case defined by 1 = 7 , 1 / P =
0 ...
Page 159
The correct procedure is to average for a sufficient number of small crystals with
N lattice sites containing an average of No defects . Among the various
mathematical procedures to perform this we choose for this discussion the use of
the long ...
The correct procedure is to average for a sufficient number of small crystals with
N lattice sites containing an average of No defects . Among the various
mathematical procedures to perform this we choose for this discussion the use of
the long ...
Page 248
A correlation between Vph and N ( 0 ) for hcp and bcc transition metals is shown
in Fig . 12 . Using McMillan ' s model , T . has a broad maximum near a = 2 that is
obtained by decreasing the average phonon frequencies . However , this is ...
A correlation between Vph and N ( 0 ) for hcp and bcc transition metals is shown
in Fig . 12 . Using McMillan ' s model , T . has a broad maximum near a = 2 that is
obtained by decreasing the average phonon frequencies . However , this is ...
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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