Introduction to Solid State PhysicsProblems after each chapter. |
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Page 105
... increase in length of the bond between atoms n and n 1. If both bonds increase in length , the two forces on atom n will be oppositely directed . Here ẞ is the force constant . Looked at on a macroscopic . scale , the line has a linear ...
... increase in length of the bond between atoms n and n 1. If both bonds increase in length , the two forces on atom n will be oppositely directed . Here ẞ is the force constant . Looked at on a macroscopic . scale , the line has a linear ...
Page 414
... increase in the value of the resultant magnetic moment of the specimen under the action of an applied magnetic field may be imagined to take place , according to the domain theory , by two inde- pendent processes , as suggested by R ...
... increase in the value of the resultant magnetic moment of the specimen under the action of an applied magnetic field may be imagined to take place , according to the domain theory , by two inde- pendent processes , as suggested by R ...
Page 560
... increase . The increase in energy can come only from an increased stress acting on the dislocation as it pulls away from the solute atom cloud , and so the presence of the cloud strengthens the crystal . In pure crystals , the passage ...
... increase . The increase in energy can come only from an increased stress acting on the dislocation as it pulls away from the solute atom cloud , and so the presence of the cloud strengthens the crystal . In pure crystals , the passage ...
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