Introduction to Solid State Physics |
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Page 12
... simple ; ( 2 ) monoclinic , simple ; ( 3 ) monoclinic , base centered ; ( 4 ) orthorhombic , simple ; ( 5 ) orthorhombic , base centered ; ( 6 ) orthorhombic , body centered ; ( 7 ) orthohombic , face centered ; ( 8 ) hexagonal ; ( 9 ) ...
... simple ; ( 2 ) monoclinic , simple ; ( 3 ) monoclinic , base centered ; ( 4 ) orthorhombic , simple ; ( 5 ) orthorhombic , base centered ; ( 6 ) orthorhombic , body centered ; ( 7 ) orthohombic , face centered ; ( 8 ) hexagonal ; ( 9 ) ...
Page 27
... Simple cubic Body - centered cubic Face - centered cubic π / 6 ( = 0.52 ) π3 / 8 ( = 0.68 ) 2/6 ( = 0.74 ) Hexagonal close - packed Diamond π2 / 6 ( = 0.74 ) 3/16 ( 0.34 ) We may note that by experiment [ O. K. Rice , J. Chem . Phys ...
... Simple cubic Body - centered cubic Face - centered cubic π / 6 ( = 0.52 ) π3 / 8 ( = 0.68 ) 2/6 ( = 0.74 ) Hexagonal close - packed Diamond π2 / 6 ( = 0.74 ) 3/16 ( 0.34 ) We may note that by experiment [ O. K. Rice , J. Chem . Phys ...
Page 77
... simple approximation to the heat capacity . If the total number of atoms is 2N , we treat the N normal modes of the optical branch as equivalent to N simple harmonic oscillators of frequency ( Eq . 4.19 ) : 12 wo 28 + m M [ 28 / M ] ...
... simple approximation to the heat capacity . If the total number of atoms is 2N , we treat the N normal modes of the optical branch as equivalent to N simple harmonic oscillators of frequency ( Eq . 4.19 ) : 12 wo 28 + m M [ 28 / M ] ...
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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absorption alkali halides alkali metal alloy anisotropy antiferromagnetic approximation atoms axes axis Bardeen barium titanate boundary calculated charge coefficient conduction band cube Curie point Debye density diamagnetic dielectric constant diffraction diffusion dipole direction discussed dislocation displacement domains effect elastic electric field entropy equation equilibrium experimental F-center factor Fermi ferroelectric ferromagnetic free electron frequency given heat capacity holes impurity interaction interstitial ionic crystals ionized lattice constant lattice points London low temperatures magnetic field magnetic moment molecules motion nearest neighbor normal observed orbital p-n junctions parallel paramagnetic particles perovskite phonons Phys physical plane polarizability polarization positive potassium chloride potential Proc quantum range order region resonance result room temperature scattering Seitz semiconductor Shockley shown in Fig single crystal sodium chloride solids specimen spin superconducting susceptibility symmetry Table theory thermal tion unit volume valence values vector velocity wave functions x-ray zero