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 284
When , however , a particular feature of its band structure is strikingly reflected in
the physical properties of a metal , we ... They fall into two classes , the alkali
metals and the noble metals , whose atomic structures and crystal structures are
...
When , however , a particular feature of its band structure is strikingly reflected in
the physical properties of a metal , we ... They fall into two classes , the alkali
metals and the noble metals , whose atomic structures and crystal structures are
...
Page 293
Although the topology of the noble metal Fermi surfaces can lead to very complex
transport properties , the Fermi surfaces have but a single branch , and therefore
like the alkali metals the noble metals can be treated as one - band metals in ...
Although the topology of the noble metal Fermi surfaces can lead to very complex
transport properties , the Fermi surfaces have but a single branch , and therefore
like the alkali metals the noble metals can be treated as one - band metals in ...
Page 298
THE DIVALENT METALS The divalent metals lie in the columns of the periodic
table immediately to the right of the alkali ... 2 DIVALENT METALS IIA METALS
JIB METALS hcp hcp Be : 1822s2 Mg : [ Ne ] 3s2 Ca : [ Ar ] 452 Sr : [ Kr ] 5s Ba : [
Xe ] ...
THE DIVALENT METALS The divalent metals lie in the columns of the periodic
table immediately to the right of the alkali ... 2 DIVALENT METALS IIA METALS
JIB METALS hcp hcp Be : 1822s2 Mg : [ Ne ] 3s2 Ca : [ Ar ] 452 Sr : [ Kr ] 5s Ba : [
Xe ] ...
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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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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