Introduction to Solid State Physics |
From inside the book
Results 1-3 of 77
Page 74
9 ) valid for the equivalent homogeneous line . In this approximation dk ... The
upper limit to the integral , wm , is here to be determined by the condition that the
number of states considered should come out equal to N = L / a . Now km = a / a
as ...
9 ) valid for the equivalent homogeneous line . In this approximation dk ... The
upper limit to the integral , wm , is here to be determined by the condition that the
number of states considered should come out equal to N = L / a . Now km = a / a
as ...
Page 244
in electron - phonon collisions will be equal to rep as just estimated . Comparing
Tep with tpp , we see that under the conditions specified phonons in a metal may
have considerably shorter relaxation times than phonons in a dielectric solid .
in electron - phonon collisions will be equal to rep as just estimated . Comparing
Tep with tpp , we see that under the conditions specified phonons in a metal may
have considerably shorter relaxation times than phonons in a dielectric solid .
Page 304
When S = 0 , each lattice contains equal numbers of A and B atoms and there is
no long range order . We consider now that part of the internal energy associated
with AA , AB , and BB nearest neighbor bond energies , with the ultimate object ...
When S = 0 , each lattice contains equal numbers of A and B atoms and there is
no long range order . We consider now that part of the internal energy associated
with AA , AB , and BB nearest neighbor bond energies , with the ultimate object ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
13 other sections not shown
Other editions - View all
Common terms and phrases
alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero
Bibliographic information
| Title | Introduction to Solid State Physics Wiley series on the science and technology of materials |
| Author | Charles Kittel |
| Edition | 2 |
| Publisher | Wiley, 1953 |
| Original from | the University of Michigan |
| Digitized | 21 Nov 2007 |
| Length | 396 pages |
| Export Citation | BiBTeX EndNote RefMan |