Introduction to Solid State PhysicsProblems after each chapter. |
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Page 141
... problems in solid state physics . An approximate calculation has been given by Debye , 10 and Peierls11 has considered the problem in great detail . They both show that A is proportional to 1 / T at high temperatures , in agreement with ...
... problems in solid state physics . An approximate calculation has been given by Debye , 10 and Peierls11 has considered the problem in great detail . They both show that A is proportional to 1 / T at high temperatures , in agreement with ...
Page 180
... problem the cavity need not be chosen as spherical , but may be of any shape possessing at least cubic symmetry . We may for example take the cavity as a cube with a face normal parallel to the polarization . In this case the ...
... problem the cavity need not be chosen as spherical , but may be of any shape possessing at least cubic symmetry . We may for example take the cavity as a cube with a face normal parallel to the polarization . In this case the ...
Page 505
... problem and the problem of donor and accep- tor levels considered in Chapter 13. The energy levels referred to the bottom of the conduction band are given by the modified Rydberg formula ( 18.2 ) En = мед 2h2e2n2 2 The lattice ...
... problem and the problem of donor and accep- tor levels considered in Chapter 13. The energy levels referred to the bottom of the conduction band are given by the modified Rydberg formula ( 18.2 ) En = мед 2h2e2n2 2 The lattice ...
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 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