Introduction to Solid State PhysicsProblems after each chapter. |
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Page 51
... its reciprocal a bec lattice . In the direct fec lattice the distance between lattice planes in each cube edge direction is a / 2 , where a is the lattice constant ; thus there are points in the reciprocal lattice along the x , y , z ...
... its reciprocal a bec lattice . In the direct fec lattice the distance between lattice planes in each cube edge direction is a / 2 , where a is the lattice constant ; thus there are points in the reciprocal lattice along the x , y , z ...
Page 173
... its shape and on the strength of its interactions with the environment . The closer the approach to sphericity and the lower the dipole moment , the more easily the molecule will rotate . Thus solid methane ( CH4 ) , which is a ...
... its shape and on the strength of its interactions with the environment . The closer the approach to sphericity and the lower the dipole moment , the more easily the molecule will rotate . Thus solid methane ( CH4 ) , which is a ...
Page 558
... its ends where it leaves the plane . When an external stress is applied , the segment cannot glide as a whole because its ends are fixed , and the only possible motion is to bend into an are of a circle . We already have calculated the ...
... its ends where it leaves the plane . When an external stress is applied , the segment cannot glide as a whole because its ends are fixed , and the only possible motion is to bend into an are of a circle . We already have calculated 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 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