Solid State Physics |
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Page 63
... dimensional motion . However , great insight can be gained by studying a one - dimensional situation , and the analysis is much less com- plicated . 3-2 One - Dimensional Monatomic Lattice Consider the one - dimensional lattice shown in ...
... dimensional motion . However , great insight can be gained by studying a one - dimensional situation , and the analysis is much less com- plicated . 3-2 One - Dimensional Monatomic Lattice Consider the one - dimensional lattice shown in ...
Page 71
Harold T. Stokes. Let us now consider the reciprocal one - dimensional lattice . The reciprocal lattice vectors G are defined by Eq . ( 2-16 ) to be solutions to the equation , RG = 2πn . ( Since there is only one direction in one - ...
Harold T. Stokes. Let us now consider the reciprocal one - dimensional lattice . The reciprocal lattice vectors G are defined by Eq . ( 2-16 ) to be solutions to the equation , RG = 2πn . ( Since there is only one direction in one - ...
Page 153
... one dimension since it is easier to visualize . Consider a one - dimensional metal . The positive ions are separated by a distance a , the lattice parameter . In the free- electron model , the energy E of a conduction electron with wave ...
... one dimension since it is easier to visualize . Consider a one - dimensional metal . The positive ions are separated by a distance a , the lattice parameter . In the free- electron model , the energy E of a conduction electron with wave ...
Common terms and phrases
Answer atoms average bond Bragg angle Bragg's Law Bravais lattice Brillouin zone called Chapter classical model collisions conduction electrons Consider constructively interfere Cooper pairs copper depletion layer direction dispersion curve displacement distance doped effective mass elec electric current electric field electrons and holes energy band equal example fcc lattice Fermi energy Fermi level Fermi surface force free electron free particle frequency given by Eq inside ions k-space laser lattice parameter lattice points lattice vector lattice wave magnetic field n-type semiconductor Na+-Cl NaCl negative neutrons number of electrons obtain occupied one-dimensional oscillate p-n junction p-side n-side photon planes positively charged potential energy primitive unit cell Problem rays reciprocal lattice reverse biased scattered Schroedinger's equation shown in Fig sodium metal superconductor temperature thermal energy tion transistor trons unit cell unoccupied values velocity voltage wave function wave number wave vector wavelength wire x-ray diffraction zero