Solid State PhysicsThe Drude Theory of Metals. The Sommerfeld Theory of Metals. Failures of the Free Electron Model. Crystal Lattices. The Reciprocal Lattice. Determination of Crystal Structures by X-Ray Diffraction. Classification of Bravais Lattices and Crystal Structures. Electron levels in a Periodic Potential: General Properties. Electrons in a Weak Periodic Potential.THe Tight-Binding Method. Other Methods for Calculating Band Structure. The Semiclassical Model of Electron Dynamics. The Semiclassical Theory of Conduction in Metals. Measuring the Fermi Surface. Band Structure of Selected Metals. Beyond the Relaxation. Time Approximation. Beyond the Independent Electron Approximation. Surface Effects. Classification of Solids. Cohesive Energy. Failures of the Static Lattice Model. Classical Theory of the Harmonic Crystal. Quantum Theory of the Harmonic Crystal. Measuring Phonon Dispersion Relations. Anharmonic Effects in Crystals. Phonons in Metals. Dielectric Properties of Insulators. Homogeneous Semiconductors. Inhomogeneous Semiconductors. Defects in Crystals. Diamagnetism and Paramagnetism. Electron Interactions and Magnetic Structure. Magnetic Ordering. Superconductivity. Appendices. |
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Page 385
AshcroftNeil W., Neil W. Ashcroft, N. David Mermin Brooks/Cole Publishing
Company. Table 19 . 1 PROPOSED IONIC RADII FOR THE ALKALI HALIDES Li
+ ( 0 . 60 ) Na + ( 0 . 95 ) K + ( 1 . 33 ) Rb + ( 1 . 48 ) Cs + ( 1 . 69 ) F - ( 1 . 36 ) 2 .
67 2 .
AshcroftNeil W., Neil W. Ashcroft, N. David Mermin Brooks/Cole Publishing
Company. Table 19 . 1 PROPOSED IONIC RADII FOR THE ALKALI HALIDES Li
+ ( 0 . 60 ) Na + ( 0 . 95 ) K + ( 1 . 33 ) Rb + ( 1 . 48 ) Cs + ( 1 . 69 ) F - ( 1 . 36 ) 2 .
67 2 .
Page 391
It is instructive to compare the ionic radii of the metallic elements ( as calculated
from the structure of the ionic crystals they participate in ) with the nearest -
neighbor distance in the metal ( Table 19 . 4 ) . It is evident that the concept of
ionic ...
It is instructive to compare the ionic radii of the metallic elements ( as calculated
from the structure of the ionic crystals they participate in ) with the nearest -
neighbor distance in the metal ( Table 19 . 4 ) . It is evident that the concept of
ionic ...
Page 812
... use of term , 416n Ion cores , 374n See also Core - core repulsion ; Core
electrons Ionic bond , 379 , 388 Ionic conduction , 621 – 622 Ionic crystals , 377 -
379 I - VII ( alkali halides ) , 380 - 385 II - VI , 385 - 387 III - V ( mixed ionic -
covalent ) ...
... use of term , 416n Ion cores , 374n See also Core - core repulsion ; Core
electrons Ionic bond , 379 , 388 Ionic conduction , 621 – 622 Ionic crystals , 377 -
379 I - VII ( alkali halides ) , 380 - 385 II - VI , 385 - 387 III - V ( mixed ionic -
covalent ) ...
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Contents
The Drude Theory of Metals | 1 |
Free electron densities and rga | 5 |
Thermal conductivities | 21 |
Copyright | |
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additional applied approximation assume atomic band boundary Bragg Bravais lattice calculation carrier Chapter charge close collisions compared completely condition conduction consider constant containing contribution correction crystal cubic density dependence derivation described determined direction discussion distribution effect electric field elements energy equal equation equilibrium example fact Fermi surface Figure follows free electron frequency given gives heat hexagonal holes important independent integral interaction ionic ions known lattice vector leading levels limit linear magnetic field mean measured metals method momentum motion normal Note observed occupied orbits perpendicular phonon plane positive possible potential present primitive cell problem properties reciprocal lattice reflection region relation requires result satisfy scattering semiclassical Show shown simple single solid solution space specific structure symmetry Table temperature term theory thermal vanishes volume wave functions wave vector zero zone