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 79
... Note also that , when viewed along the c - axis , the two types of planes merge to form the two - dimensional honeycomb array of Figure 4.3 , which is not a Bravais lattice . Other Close - Packing Possibilities Note that the hcp ...
... Note also that , when viewed along the c - axis , the two types of planes merge to form the two - dimensional honeycomb array of Figure 4.3 , which is not a Bravais lattice . Other Close - Packing Possibilities Note that the hcp ...
Page 545
... note that the long - range electrostatic forces between ions are already contained in the field Eloc . The remaining short - range interionic forces ( e.g. , higher - order electrostatic multipole moments and core - core repulsion ) ...
... note that the long - range electrostatic forces between ions are already contained in the field Eloc . The remaining short - range interionic forces ( e.g. , higher - order electrostatic multipole moments and core - core repulsion ) ...
Page 680
... note that each individual electron spin operator satisfies S2 = ( † + 1 ) ( +1 ) , so that the total spin S satisfies · = s2 = ( S1 + S2 ) 2 = + 2S1 S2 . • 1 ( 32.17 ) Since S2 has the eigenvalue S ( S + 1 ) in states of spin S , it ...
... note that each individual electron spin operator satisfies S2 = ( † + 1 ) ( +1 ) , so that the total spin S satisfies · = s2 = ( S1 + S2 ) 2 = + 2S1 S2 . • 1 ( 32.17 ) Since S2 has the eigenvalue S ( S + 1 ) in states of spin S , it ...
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