Introduction to Solid State Physicsproblems after each chapter |
From inside the book
Results 1-3 of 60
Page 315
The zone is a possible choice of the primitive cell of a bec lattice , and so the
volume is $ ( 4x / a ) 3 = 4 ( 21 / a ) . There are then 8 / a ' states in the zone per
unit volume of crystal . A fcc crystal contains 4 / a ? atoms per unit volume , and
so we ...
The zone is a possible choice of the primitive cell of a bec lattice , and so the
volume is $ ( 4x / a ) 3 = 4 ( 21 / a ) . There are then 8 / a ' states in the zone per
unit volume of crystal . A fcc crystal contains 4 / a ? atoms per unit volume , and
so we ...
Page 316
faces of the first zone . This is essentially because the reflections from the plane
of atoms midway between the planes bounding the primitive cell will just cancel
in phase the reflections from the basal plane . We are therefore led to consider
the ...
faces of the first zone . This is essentially because the reflections from the plane
of atoms midway between the planes bounding the primitive cell will just cancel
in phase the reflections from the basal plane . We are therefore led to consider
the ...
Page 326
The observed electron concentration of the B phase ( bcc ) is close to the
concentration 1.48 for which the inscribed Fermi sphere makes contact with the
Brillouin zone surface for the bcc lattice . Contact of the Fermi sphere with the
zone ...
The observed electron concentration of the B phase ( bcc ) is close to the
concentration 1.48 for which the inscribed Fermi sphere makes contact with the
Brillouin zone surface for the bcc lattice . Contact of the Fermi sphere with the
zone ...
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 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