Introduction to Solid State Physicsproblems after each chapter |
From inside the book
Results 1-3 of 58
Page 313
The zone boundaries determined by ( 12.1 ) are planes normal to each G at the midpoint . The first Brillouin zone will be formed from the shortest G's , of which there are twelve given by ( 12.7 ) . The zone is therefore the rhombic ...
The zone boundaries determined by ( 12.1 ) are planes normal to each G at the midpoint . The first Brillouin zone will be formed from the shortest G's , of which there are twelve given by ( 12.7 ) . The zone is therefore the rhombic ...
Page 314
thus there are two states in the zone per atom , one state for each spin orientation . This result agrees with our earlier statement that an energy band contains two states for every atom in the crystal . There are several further ...
thus there are two states in the zone per atom , one state for each spin orientation . This result agrees with our earlier statement that an energy band contains two states for every atom in the crystal . There are several further ...
Page 326
Contact of the Fermi sphere with the zone boundary for the y sphere is at the concentration 1.54 , according to Jones . ... and the electron concentration at which the Fermi surface makes contact with the Brillouin zone boundary .
Contact of the Fermi sphere with the zone boundary for the y sphere is at the concentration 1.54 , according to Jones . ... and the electron concentration at which the Fermi surface makes contact with the Brillouin zone boundary .
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
Copyright | |
17 other sections not shown
Other editions - View all
Common terms and phrases
alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic magnetic field mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone