Introduction to Solid State Physicsproblems after each chapter |
From inside the book
Results 1-3 of 88
Page 85
Polycrystalline specimens may have isotropic elastic properties and may be
described approximately by fewer elastic constants than a single crystal , but the
values of the constants for single crystals are of fundamental significance . We
shall ...
Polycrystalline specimens may have isotropic elastic properties and may be
described approximately by fewer elastic constants than a single crystal , but the
values of the constants for single crystals are of fundamental significance . We
shall ...
Page 312
12 Application of Brillouin Zone Theory to Metals and Alloys In this chapter we
shall apply band theory in a descriptive and qualitative way to account for a
number of physical properties of metals and alloys . We shall be concerned in the
main ...
12 Application of Brillouin Zone Theory to Metals and Alloys In this chapter we
shall apply band theory in a descriptive and qualitative way to account for a
number of physical properties of metals and alloys . We shall be concerned in the
main ...
Page 347
At absolute zero a pure and perfect crystal of most semiconductors would behave
as an insulator ; the characteristic semiconducting properties are usually brought
about by thermal agitation , impurities , or lattice defects . A number of devices ...
At absolute zero a pure and perfect crystal of most semiconductors would behave
as an insulator ; the characteristic semiconducting properties are usually brought
about by thermal agitation , impurities , or lattice defects . A number of devices ...
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 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