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. |
From inside the book
Results 1-3 of 71
Page 379
IONIC CRYSTALS The most naive model of an ionic crystal treats all ions as
impenetrable charged spheres . ... impenetrability is a consequence of the Pauli
exclusion principle and the stable closed - shell electronic configurations of the
ions .
IONIC CRYSTALS The most naive model of an ionic crystal treats all ions as
impenetrable charged spheres . ... impenetrability is a consequence of the Pauli
exclusion principle and the stable closed - shell electronic configurations of the
ions .
Page 383
which the ions are regarded as impenetrable spheres of a definite radius r ,
known as the ionic radius . Let d be the distance between the centers of
neighboring positive and negative ions , so that d = a / 2 in the sodium chloride
structure , and ...
which the ions are regarded as impenetrable spheres of a definite radius r ,
known as the ionic radius . Let d be the distance between the centers of
neighboring positive and negative ions , so that d = a / 2 in the sodium chloride
structure , and ...
Page 416
In subsequent chapters the periodic array of ions has played a critical role in our
treatment of metals and insulators . In all such discussions we have taken the
ions to constitute a fixed , rigid , immobile periodic array . 2 This , however , is
only ...
In subsequent chapters the periodic array of ions has played a critical role in our
treatment of metals and insulators . In all such discussions we have taken the
ions to constitute a fixed , rigid , immobile periodic array . 2 This , however , is
only ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
The Drude Theory of Metals | 1 |
Free electron densities and rga | 5 |
Electrical resistivities | 8 |
Copyright | |
34 other sections not shown
Other editions - View all
Common terms and phrases
additional applied approximation assume atomic band boundary Bragg Bravais lattice calculation carrier Chapter charge close collisions compared 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