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 215
Justifying the semiclassical model in detail is a formidable task , considerably
more difficult than justifying the ordinary ... for the semiclassical model is urged to
examine the broad array of mysteries and anomalies of free electron theory that ...
Justifying the semiclassical model in detail is a formidable task , considerably
more difficult than justifying the ordinary ... for the semiclassical model is urged to
examine the broad array of mysteries and anomalies of free electron theory that ...
Page 217
The semiclassical model describes the response of the electrons to externally
applied electric and magnetic fields that vary slowly over the dimensions of such
a wave packet ( Figure 12 . 1 ) and therefore exceedingly slowly over a few ...
The semiclassical model describes the response of the electrons to externally
applied electric and magnetic fields that vary slowly over the dimensions of such
a wave packet ( Figure 12 . 1 ) and therefore exceedingly slowly over a few ...
Page 222
The semiclassical equations ( 12 . 6 ) imply that a filled band remains a filled
band at all times , even in the presence of space - and time - dependent electric
and magnetic fields . This is a direct consequence of the semiclassical analogue
of ...
The semiclassical equations ( 12 . 6 ) imply that a filled band remains a filled
band at all times , even in the presence of space - and time - dependent electric
and magnetic fields . This is a direct consequence of the semiclassical analogue
of ...
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Contents
The Drude Theory of Metals | 1 |
Free electron densities and rga | 5 |
Electrical resistivities | 8 |
Copyright | |
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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