Introduction to Solid State Physicsproblems after each chapter |
From inside the book
Results 1-3 of 90
Page xix
A perfect crystal is considered to be constructed by the infinite regular repetition
in space of identical structural units or building blocks . We give in this chapter an
introductory discussion of the essential symmetry properties of crystal structures ...
A perfect crystal is considered to be constructed by the infinite regular repetition
in space of identical structural units or building blocks . We give in this chapter an
introductory discussion of the essential symmetry properties of crystal structures ...
Page 103
Lattice Vibrations In this chapter we discuss the elastic vibrations of crystals . We
extend the discussion of the preceding chapter to the short wavelength range ,
where the wavelength of the lattice wave is comparable with the lattice constant
of ...
Lattice Vibrations In this chapter we discuss the elastic vibrations of crystals . We
extend the discussion of the preceding chapter to the short wavelength range ,
where the wavelength of the lattice wave is comparable with the lattice constant
of ...
Page 241
The mobility is a particularly useful quantity in dealing with semiconductors ,
Chapter 13 . We have quoted ( but not yet derived ) the value 1 . 6 X 108 cm / sec
for the intrinsic velocity of the conduction electrons in copper . The drift velocity ...
The mobility is a particularly useful quantity in dealing with semiconductors ,
Chapter 13 . We have quoted ( but not yet derived ) the value 1 . 6 X 108 cm / sec
for the intrinsic velocity of the conduction electrons in copper . The drift velocity ...
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 axes 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