Electronic Structure and PropertiesFrank Y. Fradin |
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Page 167
... velocity is ħk F / m where ħk is the Fermi momentum and m is the effective mass in the absence of electron - phonon interactions . The Fermi momentum is not affected by the electron - phonon interaction so that the velocity reduc- tion ...
... velocity is ħk F / m where ħk is the Fermi momentum and m is the effective mass in the absence of electron - phonon interactions . The Fermi momentum is not affected by the electron - phonon interaction so that the velocity reduc- tion ...
Page 234
... velocity ; or ( ii ) the projection of the strain momentum onto the velocity of the state equals the deformation potential . A scattering picture emerges , in that the strain changes the kinematics of electrons ; the first - order ...
... velocity ; or ( ii ) the projection of the strain momentum onto the velocity of the state equals the deformation potential . A scattering picture emerges , in that the strain changes the kinematics of electrons ; the first - order ...
Page 317
... velocity of these states is lower than that of the bands made of predominantly s and p states . Similarly , the effective masses are , in general , considerably higher . In a solid made up of overlapping sp and d bands an electrical ...
... velocity of these states is lower than that of the bands made of predominantly s and p states . Similarly , the effective masses are , in general , considerably higher . In a solid made up of overlapping sp and d bands an electrical ...
Contents
Photoelectron Spectroscopy as an Electronic | 99 |
Electronic Structure and the ElectronPhonon Interaction | 165 |
Elastic Properties of Transition Metals | 223 |
Copyright | |
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Electronic Structure and Properties: Treatise on Materials ..., Volume 21 Frank Y. Fradin Limited preview - 2016 |
Common terms and phrases
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