Introduction to Solid State PhysicsProblems after each chapter. |
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Page 75
... negative ions at p = 2 , giving - 12/2 ; eight positive ions at p = 3 , giving 8/32 ; six negative ions at p = 2 , giving - ; etc. , and so απ 6 12 8 + - 1 22 3 = 6.000 - - 6 + 2 8.4854.620 - 3.000 + The convergence is obviously poor ...
... negative ions at p = 2 , giving - 12/2 ; eight positive ions at p = 3 , giving 8/32 ; six negative ions at p = 2 , giving - ; etc. , and so απ 6 12 8 + - 1 22 3 = 6.000 - - 6 + 2 8.4854.620 - 3.000 + The convergence is obviously poor ...
Page 300
... negative charge and negative mass . The following consideration shows that only the positive possibility is correct . - – If the band were entirely filled the total velocity summed over every electron in the band would be zero : a ...
... negative charge and negative mass . The following consideration shows that only the positive possibility is correct . - – If the band were entirely filled the total velocity summed over every electron in the band would be zero : a ...
Page 542
... Negative dislocation Motion of a dislocation under a shear tending to move the upper surface of the specimen to the right . Above , a positive dislocation moves from left to right ; below , a negative dislocation moves from right to ...
... Negative dislocation Motion of a dislocation under a shear tending to move the upper surface of the specimen to the right . Above , a positive dislocation moves from left to right ; below , a negative dislocation moves from right to ...
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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absorption acceptors alkali alloys approximately atoms axes axis barium titanate boundary Bragg Brillouin zone calculated chapter charge conduction band conduction electrons crystal structure cube cubic Curie point Debye density dielectric constant diffraction diffusion dipole direction discussion dislocation distribution domain effective mass elastic electric field energy equation equilibrium exciton experimental F centers factor Fermi ferroelectric ferromagnetic free electron frequency germanium given heat capacity hexagonal holes impurity interaction ionization ions lattice constant lattice point low temperatures magnetic field magnetic moment metals molecules motion nearest neighbor normal observed p-n junction paramagnetic particles phonons Phys physics plane polarizability polarization positive potential Proc resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory thermal tion transistor transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero