Electronic Structure and PropertiesFrank Y. Fradin |
From inside the book
Results 1-3 of 89
Page 3
... measured electron masses , electron velocities , g factors , the measured oscillator strength for optical transitions , density of states at the Fermi energy as obtained from specific heat measurements , etc. In general , it does not ...
... measured electron masses , electron velocities , g factors , the measured oscillator strength for optical transitions , density of states at the Fermi energy as obtained from specific heat measurements , etc. In general , it does not ...
Page 114
... measured kinetic energy is E = E ( k ) - Evac and E ; ( k ) = E ( k ) – hv , - ( 5 ) so that knowledge of Evac and hy specifies both E , and E , at the measured ✪ ( the collection angle relative to the surface normal ) . Knowledge of 0 ...
... measured kinetic energy is E = E ( k ) - Evac and E ; ( k ) = E ( k ) – hv , - ( 5 ) so that knowledge of Evac and hy specifies both E , and E , at the measured ✪ ( the collection angle relative to the surface normal ) . Knowledge of 0 ...
Page 341
... measured by platinum resistance thermometry . In practice , point - by - point sample resistance measurements are taken as the temperature was slowly swept both up and down . The rate of change of temperature should be kept slow enough ...
... measured by platinum resistance thermometry . In practice , point - by - point sample resistance measurements are taken as the temperature was slowly swept both up and down . The rate of change of temperature should be kept slow enough ...
Contents
Photoelectron Spectroscopy as an Electronic | 99 |
Electronic Structure and the ElectronPhonon Interaction | 165 |
Elastic Properties of Transition Metals | 223 |
Copyright | |
11 other sections not shown
Other editions - View all
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