Introduction to Solid State PhysicsProblems after each chapter. |
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Page 88
... applied . Thus the stress component X , represents a force applied in the x direc- tion to a unit area of a plane whose normal lies in the direction ; the stress com- ponent X , represents a force applied in the direction to a unit area ...
... applied . Thus the stress component X , represents a force applied in the x direc- tion to a unit area of a plane whose normal lies in the direction ; the stress com- ponent X , represents a force applied in the direction to a unit area ...
Page 180
... applied field is in the x direction , then the x component of the field of the nucleus at the displaced position of the electron orbit must be equal to the applied field . The correct quantum - mechanical result is larger than this by ...
... applied field is in the x direction , then the x component of the field of the nucleus at the displaced position of the electron orbit must be equal to the applied field . The correct quantum - mechanical result is larger than this by ...
Page 387
... applied in " forward " direction ( b ) Voltage V applied in " back " direction Fig . 14.5 . Effect of an applied voltage on the current flow through the contact of Fig . 14.4 , exhibiting the origin of rectification . In ( a ) the ...
... applied in " forward " direction ( b ) Voltage V applied in " back " direction Fig . 14.5 . Effect of an applied voltage on the current flow through the contact of Fig . 14.4 , exhibiting the origin of rectification . In ( a ) 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