Introduction to Solid State Physics |
From inside the book
Results 1-3 of 13
Page 320
An exciton 15 or excitation wave is produced when an insulator is raised to the
first non - conducting excited state of its electronic system . The first electronic
transition is called the first fundamental absorption band of the crystal . It is
centered ...
An exciton 15 or excitation wave is produced when an insulator is raised to the
first non - conducting excited state of its electronic system . The first electronic
transition is called the first fundamental absorption band of the crystal . It is
centered ...
Page 315
The initial excitation may be by light , electron or positive ion bombardment ,
mechanical strain , chemical reaction , or heating . If the emission occurs during
excitation , or within 10 - 8 sec of excitation , the substituting for p ( r ) and
carrying out ...
The initial excitation may be by light , electron or positive ion bombardment ,
mechanical strain , chemical reaction , or heating . If the emission occurs during
excitation , or within 10 - 8 sec of excitation , the substituting for p ( r ) and
carrying out ...
Page 320
An exciton 15 or excitation wave is produced when an insulator is raised to the
first non - conducting excited state of its electronic system . The first electronic
transition is called the first fundamental absorption band of the crystal . It is
centered ...
An exciton 15 or excitation wave is produced when an insulator is raised to the
first non - conducting excited state of its electronic system . The first electronic
transition is called the first fundamental absorption band of the crystal . It is
centered ...
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