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 12
An electric field Ex is applied to a wire extending in the x - direction and a current
density ją flows in the wire . In addition , a magnetic field H points in the positive z
- direction . As a result the Lorentz force16 - - v * H ( 1 . 13 ) acts to deflect ...
An electric field Ex is applied to a wire extending in the x - direction and a current
density ją flows in the wire . In addition , a magnetic field H points in the positive z
- direction . As a result the Lorentz force16 - - v * H ( 1 . 13 ) acts to deflect ...
Page 441
Note that the two transverse branches are degenerate in the [ 100 ] direction . ...
not only the behavior of the frequencies ws ( k ) , but also the relations between
the directions of the polarization vectors ez ( k ) and the direction of propagation k
.
Note that the two transverse branches are degenerate in the [ 100 ] direction . ...
not only the behavior of the frequencies ws ( k ) , but also the relations between
the directions of the polarization vectors ez ( k ) and the direction of propagation k
.
Page 474
If we only examine neutrons emerging in a definite direction we will specify the
direction of p ' , and can therefore expect to find solutions at only a single point on
the surface ( or a finite number of points on the surfaces ) . If we select a general ...
If we only examine neutrons emerging in a definite direction we will specify the
direction of p ' , and can therefore expect to find solutions at only a single point on
the surface ( or a finite number of points on the surfaces ) . If we select a general ...
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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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Solid State Physics: Advances in Research and Applications, Volume 42 Henry Ehrenreich Limited preview - 1989 |
Common terms and phrases
additional applied approximation assume atomic band boundary Bragg Bravais lattice calculation carrier Chapter charge close collisions compared completely 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