Introduction to Solid State PhysicsProblems after each chapter. |
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Page 27
... usually chosen as the unit cell . The lattice is primitive , but it is usually denoted by R , rather than P , so that we speak of the trigonal R space lattice . Fig . 1.13 . Primitive translation vectors of the body - centered cubic I ...
... usually chosen as the unit cell . The lattice is primitive , but it is usually denoted by R , rather than P , so that we speak of the trigonal R space lattice . Fig . 1.13 . Primitive translation vectors of the body - centered cubic I ...
Page 164
... usually be separated into three parts : electronic , ionic , and orientational . The electronic contribution arises ... usually also an interfacial polarization arising from the accumulation of charge at structural interfaces . This is ...
... usually be separated into three parts : electronic , ionic , and orientational . The electronic contribution arises ... usually also an interfacial polarization arising from the accumulation of charge at structural interfaces . This is ...
Page 415
... usually proceed by means of domain boundary displacements , and so the domains change in size . In strong fields the magnetization usually changes by means of rotation of the direction of magnetization . A typical magnetization curve is ...
... usually proceed by means of domain boundary displacements , and so the domains change in size . In strong fields the magnetization usually changes by means of rotation of the direction of magnetization . A typical magnetization curve is ...
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