Introduction to Solid State Physicsproblems after each chapter |
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Page 293
61 ) X8 a m * . The proportionality of the heat capacity and spin susceptibility to m
* reflects directly the proportionality of the density of states at the top 8 . 0 x 10 - 6
r 12 x. s Representative treatments include those by G . H . Wannier , Phys .
61 ) X8 a m * . The proportionality of the heat capacity and spin susceptibility to m
* reflects directly the proportionality of the density of states at the top 8 . 0 x 10 - 6
r 12 x. s Representative treatments include those by G . H . Wannier , Phys .
Page 442
Phys . 18 , 1455 ( 1950 ) . 31 T . Nagamiya , Progr . Theoret . Phys . ( Japan ) 6 ,
342 ( 1951 ) ; C . Kittel , Phys . Rev . 82 , 565 ( 1951 ) ; F . Keffer and C . Kittel ,
Phys . Rev . 86 , 329 ( 1952 ) ; F . Keffer , Phys . Rev . 87 , 608 ( 1952 ) . 32 Poulis
...
Phys . 18 , 1455 ( 1950 ) . 31 T . Nagamiya , Progr . Theoret . Phys . ( Japan ) 6 ,
342 ( 1951 ) ; C . Kittel , Phys . Rev . 82 , 565 ( 1951 ) ; F . Keffer and C . Kittel ,
Phys . Rev . 86 , 329 ( 1952 ) ; F . Keffer , Phys . Rev . 87 , 608 ( 1952 ) . 32 Poulis
...
Page 509
The spectrum of crystalline phenanthrene C14H10 is shown in Fig . 18 . 6 . Apker
and Taft ? have carried out some very interesting optical and 6 See , for example
, the discussion of solid benzene by D . Fox and ( ) . Schnepp , J . Chem . Phys .
The spectrum of crystalline phenanthrene C14H10 is shown in Fig . 18 . 6 . Apker
and Taft ? have carried out some very interesting optical and 6 See , for example
, the discussion of solid benzene by D . Fox and ( ) . Schnepp , J . Chem . Phys .
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic magnetic field mass material measurements metals method motion neighbor normal observed obtained parallel particles Phys physics plane polarization positive possible potential problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone