Introduction to Solid State Physics |
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Page 6
... METAL CRYSTALS Metals are characterized by high electrical conductivity , so that a portion of the electrons in a metal must be free to move about . The electrons available to participate in the conductivity are called con- duction ...
... METAL CRYSTALS Metals are characterized by high electrical conductivity , so that a portion of the electrons in a metal must be free to move about . The electrons available to participate in the conductivity are called con- duction ...
Page 240
... METALS AT 18 ° C ( Values in parentheses are at 0 ° C . ) Metal Ohm - cm X 106 Metal Ohm - cm X 106 Metal Ohm - cm X 106 Li 9.1 Zr 45.0 Cu 1.68 Na 4.6 Hf 32.0 Ag 1.58 K 6.9 Та 14.7 Au 2.21 Rb 12.6 Cr ( 2.6 ) Zn 5.95 Cs 20.8 Mo 4.72 Cd ...
... METALS AT 18 ° C ( Values in parentheses are at 0 ° C . ) Metal Ohm - cm X 106 Metal Ohm - cm X 106 Metal Ohm - cm X 106 Li 9.1 Zr 45.0 Cu 1.68 Na 4.6 Hf 32.0 Ag 1.58 K 6.9 Та 14.7 Au 2.21 Rb 12.6 Cr ( 2.6 ) Zn 5.95 Cs 20.8 Mo 4.72 Cd ...
Page 268
... METALS The alkali atoms have an s valence electron on each atom : 2s in lithium , 3s in sodium , 4s in potassium , 5s in rubidium , and 6s in cesium . In the metal the s levels are ... metals do conduct electricity 268 BAND THEORY OF METALS.
... METALS The alkali atoms have an s valence electron on each atom : 2s in lithium , 3s in sodium , 4s in potassium , 5s in rubidium , and 6s in cesium . In the metal the s levels are ... metals do conduct electricity 268 BAND THEORY OF METALS.
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