Introduction to Solid State Physics |
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Page 259
BRILLOUIN ZONES We have seen , from the Kronig - Penney problem and from
Appendix L , that the energy discontinuities in ... The line segments are known as
Brillouin zones ; the segment – a / a < k < a / a is the first Brillouin zone ; the two ...
BRILLOUIN ZONES We have seen , from the Kronig - Penney problem and from
Appendix L , that the energy discontinuities in ... The line segments are known as
Brillouin zones ; the segment – a / a < k < a / a is the first Brillouin zone ; the two ...
Page 261
The outer boundary of the second zone is determined by setting ni = + 1 , n2 = +
1 , obtaining the equations of the four ... A method of treating other lattices is
given in Appendix N , along with a brief mention of the zone theory explanation of
the ...
The outer boundary of the second zone is determined by setting ni = + 1 , n2 = +
1 , obtaining the equations of the four ... A method of treating other lattices is
given in Appendix N , along with a brief mention of the zone theory explanation of
the ...
Page 262
8 suggests that the electrons might begin to populate states in the second zone
or band before filling the corners of the first zone . If we estimate energies on the
free electron model , we find that the kinetic energy of an electron at a corner of ...
8 suggests that the electrons might begin to populate states in the second zone
or band before filling the corners of the first zone . If we estimate energies on the
free electron model , we find that the kinetic energy of an electron at a corner of ...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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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