Introduction to Solid State PhysicsProblems after each chapter. |
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Page 510
... present . [ After L. Apker and E. Taft , Phys . Rev. 79 , 964 ( 1950 ) . ] threshold is observed starting at about 2 ... present . With the F centers present one observes the broad excitation curve already mentioned and also a 510 ...
... present . [ After L. Apker and E. Taft , Phys . Rev. 79 , 964 ( 1950 ) . ] threshold is observed starting at about 2 ... present . With the F centers present one observes the broad excitation curve already mentioned and also a 510 ...
Page 524
... present in only small propor- tions ; there are also a number of pure materials which luminesce efficiently . Phosphorescent crystals may be divided into two classes : photoconductors of which Cu - activated ZnS is the prototype , and ...
... present in only small propor- tions ; there are also a number of pure materials which luminesce efficiently . Phosphorescent crystals may be divided into two classes : photoconductors of which Cu - activated ZnS is the prototype , and ...
Page 557
... present , lattice vacancies pre- cipitating along its length will eat away a portion of the extra half- plane of atoms and cause the dislocation to climb , or move at right angles to its slip direction . If no edge dislocations are present ...
... present , lattice vacancies pre- cipitating along its length will eat away a portion of the extra half- plane of atoms and cause the dislocation to climb , or move at right angles to its slip direction . If no edge dislocations are present ...
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 levels 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