Introduction to Solid State PhysicsProblems after each chapter. |
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Page 88
... tion to a unit area of a plane whose normal lies in the direction ; the stress com- ponent X , represents a force ... tion that the angular acceleration vanish , and hence that the total torque must be zero . It follows that Fig . 4.2 ...
... tion to a unit area of a plane whose normal lies in the direction ; the stress com- ponent X , represents a force ... tion that the angular acceleration vanish , and hence that the total torque must be zero . It follows that Fig . 4.2 ...
Page 236
... tion , the approach to equilibrium is described by the appropriate solu- tion of ( 10.3 ) : ( 10.4 ) VD ( 1 ) = VD ( 0 ) e ̄t / . We have thus arranged things so that a disturbance from equilibrium dies out exponentially , with the ...
... tion , the approach to equilibrium is described by the appropriate solu- tion of ( 10.3 ) : ( 10.4 ) VD ( 1 ) = VD ( 0 ) e ̄t / . We have thus arranged things so that a disturbance from equilibrium dies out exponentially , with the ...
Page 520
... tion at 0.78 ev . It is known that 0.38 ev corresponds to the energy required to free one trapped hole from a Mn atom in germanium ; so we may suppose that the release of holes to the valence band increases the recombina- tion of the ...
... tion at 0.78 ev . It is known that 0.38 ev corresponds to the energy required to free one trapped hole from a Mn atom in germanium ; so we may suppose that the release of holes to the valence band increases the recombina- tion of the ...
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