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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Results 1-3 of 66
Page 226
where the integral is over all occupied levels in the band . ... Thus the current
produced by occupying with electrons a specified set of levels is precisely the
same as the current that would be produced if ( a ) the specified levels were ...
where the integral is over all occupied levels in the band . ... Thus the current
produced by occupying with electrons a specified set of levels is precisely the
same as the current that would be produced if ( a ) the specified levels were ...
Page 234
Because & ( k ) is very close to & ( k ) , we shall assume that whichever of these
criteria is satisfied by the orbits determined by Ē is also satisfied by the orbits
determined by E . Case 1 When all occupied ( or all unoccupied ) orbits are
closed ...
Because & ( k ) is very close to & ( k ) , we shall assume that whichever of these
criteria is satisfied by the orbits determined by Ē is also satisfied by the orbits
determined by E . Case 1 When all occupied ( or all unoccupied ) orbits are
closed ...
Page 356
Suppose that we could represent the ionic configuration by simply occupying
some finite region V of the Bravais lattice occupied in the infinite crystal .
Suppose , furthermore , that the electronic charge density in the Wigner - Seitz
cell about ...
Suppose that we could represent the ionic configuration by simply occupying
some finite region V of the Bravais lattice occupied in the infinite crystal .
Suppose , furthermore , that the electronic charge density in the Wigner - Seitz
cell about ...
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Contents
The Drude Theory of Metals | 1 |
Free electron densities and ra | 5 |
Thermal conductivities | 21 |
Copyright | |
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Common terms and phrases
additional applied approximation assume atomic band Bragg Bravais lattice calculation carrier cell centered Chapter charge classical close collisions compared condition conduction consider constant constructed containing contribution crystal cubic density dependence described determined direction discussion distance distribution effect electric field elements energy equation equilibrium example faces fact factor Fermi surface Figure follows free electron frequency given gives heat hexagonal holes important independent integral interaction ionic ions known lattice vector leads levels limit linear magnetic field mean measured metals method normal Note observed occupied orbits perpendicular phonon plane position possible potential primitive cell Problem properties reciprocal lattice reflection region relation requires result satisfy scattering semiclassical Show shown simple single solid solution space space groups specific sphere structure symmetry Table temperature term theory thermal unit vanishes volume wave functions wave vector zone