Electronic Structure and PropertiesFrank Y. Fradin |
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Page 83
Frank Y. Fradin. 0.5 EDGE 0 UPPER PEAK- PEAK -1.5 1 2 4 6 hv ( eV ) 0 10 20 0.5 EDGE UPPER PEAK -1.5 ATOMIC PERCENT Zn ( 0 ) 30 0 10 20 30 ATOMIC PERCENT Zn ( b ) SMT MODEL -SMT MODEL --- CR MODEL 0.30 0.90 0.30. ENERGY SHIFT ( eV ) -0.5 ...
Frank Y. Fradin. 0.5 EDGE 0 UPPER PEAK- PEAK -1.5 1 2 4 6 hv ( eV ) 0 10 20 0.5 EDGE UPPER PEAK -1.5 ATOMIC PERCENT Zn ( 0 ) 30 0 10 20 30 ATOMIC PERCENT Zn ( b ) SMT MODEL -SMT MODEL --- CR MODEL 0.30 0.90 0.30. ENERGY SHIFT ( eV ) -0.5 ...
Page 86
... peaks in pure Ni , which occur at these energies . In Cuo.50 Nio.so there is a broad structureless Ni peak that extends from EF to 0.12 Ry below EF and a more structured Cu peak that extends from 0.15 to 0.35 Ry below Ep . The Ni peak ...
... peaks in pure Ni , which occur at these energies . In Cuo.50 Nio.so there is a broad structureless Ni peak that extends from EF to 0.12 Ry below EF and a more structured Cu peak that extends from 0.15 to 0.35 Ry below Ep . The Ni peak ...
Page 151
... peak in UO2 near EF is associated with U 5f electrons . ( After Veal and Lam , 1974a . ) As seen in Fig . 45 , the 5f - electron peak intensity exhibits a systematic dependence on the degree of oxidation of the uranium atom ( Veal and ...
... peak in UO2 near EF is associated with U 5f electrons . ( After Veal and Lam , 1974a . ) As seen in Fig . 45 , the 5f - electron peak intensity exhibits a systematic dependence on the degree of oxidation of the uranium atom ( Veal and ...
Contents
Photoelectron Spectroscopy as an Electronic | 99 |
Electronic Structure and the ElectronPhonon Interaction | 165 |
Elastic Properties of Transition Metals | 223 |
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Electronic Structure and Properties: Treatise on Materials ..., Volume 21 Frank Y. Fradin Limited preview - 2016 |
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alloys anomalies appears approach approximation atom band structure calculated changes charge charge density compared component compounds conduction contribution corresponding crystal curve defect density dependence derivatives described determined direction discussed distribution e/at effect elastic constants electrical electron electron-phonon electronic structure elements energy et al example excitation expected experiment experimental Fermi surface field Freeman function given gives hydrogen important impurity increase indicate interaction ions Jena lattice Lett magnetic materials measured metals method negative normal noted observed obtained peak phase phonon Phys Physics positive positron potential properties proton recent region relative resistivity respectively response sample scattering shear shift shown in Fig shows similar solid solutions strain Table temperature term theoretical theory tion transition transition metals vacancy values variation void volume wave York