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 68
... example , has the form P 2a , + a2 + a3 . = a2 a3 Another equally important example is the face - centered cubic ( fcc ) Bravais lattice . To construct the face - centered cubic Bravais lattice add to the simple cubic lattice of Figure ...
... example , has the form P 2a , + a2 + a3 . = a2 a3 Another equally important example is the face - centered cubic ( fcc ) Bravais lattice . To construct the face - centered cubic Bravais lattice add to the simple cubic lattice of Figure ...
Page 112
... examples already described that Bravais lattices do fall naturally into categories on the basis of symmetries other than translational . Simple hexagonal Bravais lattices , for example , regardless of the c / a ratio , bear a closer ...
... examples already described that Bravais lattices do fall naturally into categories on the basis of symmetries other than translational . Simple hexagonal Bravais lattices , for example , regardless of the c / a ratio , bear a closer ...
Page 396
... example , it might be convenient to define the cohesive energy of solid nitrogen as that required to separate it into a set of isolated nitrogen molecules , rather than atoms . Knowing the binding energy of an isolated nitrogen molecule ...
... example , it might be convenient to define the cohesive energy of solid nitrogen as that required to separate it into a set of isolated nitrogen molecules , rather than atoms . Knowing the binding energy of an isolated nitrogen molecule ...
Contents
The Drude Theory of Metals | 1 |
Failures of the Free Electron Model | 57 |
Crystal Lattices | 63 |
Copyright | |
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alkali atomic band structure Bloch Bragg plane Bravais lattice Brillouin zone calculation carrier densities Chapter charge density coefficients collision conduction band conduction electrons contribution crystal momentum crystal structure density of levels dependence depletion layer described dielectric constant direction distribution Drude Drude model effect electric field electron gas electron-electron electronic levels electrostatic energy gap example Fermi energy Fermi surface Figure free electron frequency given Hamiltonian hexagonal holes impurity independent electron approximation insulators interaction ionic crystals k-space lattice planes lattice point linear low temperatures macroscopic magnetic field metals neutron normal modes number of electrons one-electron levels orbits periodic potential perpendicular phonon Phys positive primitive cell primitive vectors Problem properties quantum reciprocal lattice vector region result scattering Schrödinger equation semiclassical semiconductors simple cubic solid solution specific heat spin superconducting symmetry term theory valence band vanishes velocity wave functions wave vector zero