Introduction to Solid State PhysicsProblems after each chapter. |
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Page 273
... potential energy of a conduction electron in the field of the positive ion cores of a monatomic linear lattice . We expect the ion cores to bear a positive charge , as V , potential energy ( a ) ( b ) | e || 2 , charge density α -Plane ...
... potential energy of a conduction electron in the field of the positive ion cores of a monatomic linear lattice . We expect the ion cores to bear a positive charge , as V , potential energy ( a ) ( b ) | e || 2 , charge density α -Plane ...
Page 571
... potential ( A.1 ) 4 = 41 +42 at an ion as the sum of two distinct but related potentials . The potential is that of a structure with a Gaussian distribution of charge situated at each ion site , with signs the same as those of the real ...
... potential ( A.1 ) 4 = 41 +42 at an ion as the sum of two distinct but related potentials . The potential is that of a structure with a Gaussian distribution of charge situated at each ion site , with signs the same as those of the real ...
Page 574
... potential of the charge distribution p = ( n / m ) 31⁄2 e ̄nr2 about each lattice point . By a well - known relation in electrostatics we obtain the potential of an array of unit dipoles pointing in the z direction by taking -d / dz of ...
... potential of the charge distribution p = ( n / m ) 31⁄2 e ̄nr2 about each lattice point . By a well - known relation in electrostatics we obtain the potential of an array of unit dipoles pointing in the z direction by taking -d / dz of ...
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 region resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory tion transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero