Introduction to Solid State PhysicsProblems after each chapter. |
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Page 106
... values of k merely reproduce motions already described by values of k within the limits km . If we should encounter a value of k outside these limits , we handle it by subtracting the appropriate integral mul- tiple of 2π / a which will ...
... values of k merely reproduce motions already described by values of k within the limits km . If we should encounter a value of k outside these limits , we handle it by subtracting the appropriate integral mul- tiple of 2π / a which will ...
Page 249
... values must then be filled up to ( 10.41 ) ( 8π / 3 ) nμ3 = NL3 , and so ( 10.42 ) ( np / L ) 2 = ( 3N / 8π ) 3 ... Values of the Fermi energy on the free electron model are given in Table 10.3 , together with values of the effective ...
... values must then be filled up to ( 10.41 ) ( 8π / 3 ) nμ3 = NL3 , and so ( 10.42 ) ( np / L ) 2 = ( 3N / 8π ) 3 ... Values of the Fermi energy on the free electron model are given in Table 10.3 , together with values of the effective ...
Page 295
... values of m * / m >> 1 , and to have high electronic heat capacities and high paramagnetic susceptibilities . High ... values of the magnetic susceptibility of transition elements is given in Table 11.1 ; values for the alkali metals ...
... values of m * / m >> 1 , and to have high electronic heat capacities and high paramagnetic susceptibilities . High ... values of the magnetic susceptibility of transition elements is given in Table 11.1 ; values for the alkali metals ...
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