Introduction to Solid State PhysicsProblems after each chapter. |
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Page 128
... unit volume . We have seen above that there are k3 / 2 modes per unit volume having wave vector less than k , so that the maximum km appropriate to 3N modes is given by or 3 km3 / 2m2 = 3N , km = ( 6π2N ) . ( 6.27 ) In terms of the ...
... unit volume . We have seen above that there are k3 / 2 modes per unit volume having wave vector less than k , so that the maximum km appropriate to 3N modes is given by or 3 km3 / 2m2 = 3N , km = ( 6π2N ) . ( 6.27 ) In terms of the ...
Page 258
Charles Kittel. energy per unit volume is given by ( 10.82 ) Setting ( 10.83 ) U = [ * Eƒ ( E ) g ( E ) dE . E F ( E ) ... unit volume , ( 10.86 ) 2 π Co = g [ Er ( 0 ) ] k2T . 3 Now , from ( 10.47 ) and ( 10.66 ) , ( 10.87 ) so that ...
Charles Kittel. energy per unit volume is given by ( 10.82 ) Setting ( 10.83 ) U = [ * Eƒ ( E ) g ( E ) dE . E F ( E ) ... unit volume , ( 10.86 ) 2 π Co = g [ Er ( 0 ) ] k2T . 3 Now , from ( 10.47 ) and ( 10.66 ) , ( 10.87 ) so that ...
Page 313
... unit vectors parallel to the cube edges . The volume of the prim- itive cell is ( 12.3 ) V = a . bxc = 4a3 ; we see that this is correct because the unit cube of volume a3 contains two lattice points . The primitive translations a * , b ...
... unit vectors parallel to the cube edges . The volume of the prim- itive cell is ( 12.3 ) V = a . bxc = 4a3 ; we see that this is correct because the unit cube of volume a3 contains two lattice points . The primitive translations a * , b ...
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