Introduction to Solid State Physics |
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Page 2
CLASSIFICATION OF CRYSTAL TYPES The binding energy is the energy
necessary to dissociate the solid into separated atoms , molecules , or ions , as
appropriate . The binding energy is taken at room temperature , except for the
molecular ...
CLASSIFICATION OF CRYSTAL TYPES The binding energy is the energy
necessary to dissociate the solid into separated atoms , molecules , or ions , as
appropriate . The binding energy is taken at room temperature , except for the
molecular ...
Page 104
8 It may be noted that internal interactions which favor one direction of mutual
orientation of adjacent molecules over the opposite direction may also tend to
eliminate the critical point displayed by ( 6 . 30 ) ; the effect is known as “
hindered ...
8 It may be noted that internal interactions which favor one direction of mutual
orientation of adjacent molecules over the opposite direction may also tend to
eliminate the critical point displayed by ( 6 . 30 ) ; the effect is known as “
hindered ...
Page 137
DIAMAGNETISM OF MOLECULES The derivation of the Larmor equation
assumes implicitly that the field direction is an axis of symmetry of the system . In
most molecular systems this condition is not satisfied , and the general theory of
Van ...
DIAMAGNETISM OF MOLECULES The derivation of the Larmor equation
assumes implicitly that the field direction is an axis of symmetry of the system . In
most molecular systems this condition is not satisfied , and the general theory of
Van ...
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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