Solid State PhysicsThis book provides an introduction to the field of solid state physics for undergraduate students in physics, chemistry, engineering, and materials science. |
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Page 34
(2.16) Thus in a three-dimensional space with Cartesian axes kx, ky, and kz (known as fe-space) the allowed wave vectors are those whose coordinates along the three axes are given by integral multiples of 2n/L. This is illustrated (in ...
(2.16) Thus in a three-dimensional space with Cartesian axes kx, ky, and kz (known as fe-space) the allowed wave vectors are those whose coordinates along the three axes are given by integral multiples of 2n/L. This is illustrated (in ...
Page 125
The 230 Space Groups We shall have mercifully little to say about the 230 space groups , except to point out that the number is larger than one might have guessed . For each crystal system one can construct a crystal structure with a ...
The 230 Space Groups We shall have mercifully little to say about the 230 space groups , except to point out that the number is larger than one might have guessed . For each crystal system one can construct a crystal structure with a ...
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 ...
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 ...
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Contents
The Drude Theory of Metals | 1 |
Failures of the Free Electron Model | 57 |
Crystal Lattices | 63 |
Copyright | |
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additional applied approximation assume atomic band Bragg Bravais lattice calculation carrier Chapter charge close collision compared condition conduction consider constant containing contribution correction crystal cubic density dependence described determined direction discussion distance distribution effect elements energy equation equilibrium example fact factor Fermi surface field Figure follows free electron frequency function give given hexagonal holes important impurity independent integral interaction ionic ions known lattice vector leading levels limit linear magnetic field mean measured metals mode momentum normal Note observed orbits periodic phonon plane positive possible potential present primitive cell Problem properties reciprocal lattice reflection region relation requires result satisfy scattering Show simple single solid solution space specific heat structure surface symmetry Table temperature term theory thermal unit vanishes volume wave functions wave vector zero zone