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 78
20 The hexagonal close - packed crystal structure . It can be viewed as two
interpenetrating simple hexagonal Bravais lattices , displaced vertically by a
distance c / 2 along the common c - axis , and displaced horizontally so that the
points of ...
20 The hexagonal close - packed crystal structure . It can be viewed as two
interpenetrating simple hexagonal Bravais lattices , displaced vertically by a
distance c / 2 along the common c - axis , and displaced horizontally so that the
points of ...
Page 79
Other Close - Packing Possibilities Note that the hcp structure is not the only way
to close - pack spheres . If the first two layers are laid down as described above ,
but the third is placed in the other set of depressions in the second - i . e . , those
...
Other Close - Packing Possibilities Note that the hcp structure is not the only way
to close - pack spheres . If the first two layers are laid down as described above ,
but the third is placed in the other set of depressions in the second - i . e . , those
...
Page 811
... 684 H - center , 625 hcp , see Hexagonal close - packed structure Heat
capacity , see Specific heat Heisenberg model , 679 - 681 anisotropic , 723
antiferromagnetic ground state , 704 , 722 antiferromagnetic spin waves , 708
ferromagnetic ...
... 684 H - center , 625 hcp , see Hexagonal close - packed structure Heat
capacity , see Specific heat Heisenberg model , 679 - 681 anisotropic , 723
antiferromagnetic ground state , 704 , 722 antiferromagnetic spin waves , 708
ferromagnetic ...
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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