Introduction to Solid State Physicsproblems after each chapter |
From inside the book
Results 1-3 of 72
Page 510
The hump in Y occurs only if F centers are present . ( After L . Apker and E . Taft ,
Phys . Rev . 79 , 964 ( 1950 ) . ) threshold is observed starting at about 2 ev
photon energy . The broad ionization is attributed to direct ionization of F centers
by ...
The hump in Y occurs only if F centers are present . ( After L . Apker and E . Taft ,
Phys . Rev . 79 , 964 ( 1950 ) . ) threshold is observed starting at about 2 ev
photon energy . The broad ionization is attributed to direct ionization of F centers
by ...
Page 529
When Cl - and Cut are present simultaneously a green emission is attributed to
Cu + ions substituted for Zn + t . The presence of CIsimply makes it possible for
Cut to enter the lattice , by the familiar argument of charge neutrality . The red ...
When Cl - and Cut are present simultaneously a green emission is attributed to
Cu + ions substituted for Zn + t . The presence of CIsimply makes it possible for
Cut to enter the lattice , by the familiar argument of charge neutrality . The red ...
Page 557
A problem is posed by the presence of dislocations in cast and annealed crystals
. No dislocations can be present in thermal equilibrium , because their energy is
much too great in comparison with the increase in entropy that they produce .
A problem is posed by the presence of dislocations in cast and annealed crystals
. No dislocations can be present in thermal equilibrium , because their energy is
much too great in comparison with the increase in entropy that they produce .
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