Introduction to Solid State Physicsproblems after each chapter |
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Results 1-3 of 81
Page 92
( After L. Hunter and S. Siegel , Phys . Rev. 61 , 84 ( 1942 ) ; F. C. Rose , Phys .
Rev. 49 , 50 ( 1936 ) . ) EXPERIMENTAL DETERMINATION OF ELASTIC
CONSTANTS The classic methods for the measurement of the elastic constants
of crystals ...
( After L. Hunter and S. Siegel , Phys . Rev. 61 , 84 ( 1942 ) ; F. C. Rose , Phys .
Rev. 49 , 50 ( 1936 ) . ) EXPERIMENTAL DETERMINATION OF ELASTIC
CONSTANTS The classic methods for the measurement of the elastic constants
of crystals ...
Page 365
The dashed line represents a – slope characteristic of lattice scattering . ( After
Conwell . ) We note here a small selection from analyses of semiconductor
materials carried out by similar methods : Germanium Silicon InSb H. Fritzsche ,
Phys .
The dashed line represents a – slope characteristic of lattice scattering . ( After
Conwell . ) We note here a small selection from analyses of semiconductor
materials carried out by similar methods : Germanium Silicon InSb H. Fritzsche ,
Phys .
Page 474
31 L. Tisza , Phys . Rev. 80 , 717 ( 1950 ) . 32 J. C. Slater , Phys . Rev. , 51 , 195 (
1937 ) ; 52 , 214 ( 1937 ) . 33 M. Born and K , C. Cheng , J. Phys . radium 9 , 249 (
1948 ) . 34 For references and a review of the Fröhlich and Bardeen theories ...
31 L. Tisza , Phys . Rev. 80 , 717 ( 1950 ) . 32 J. C. Slater , Phys . Rev. , 51 , 195 (
1937 ) ; 52 , 214 ( 1937 ) . 33 M. Born and K , C. Cheng , J. Phys . radium 9 , 249 (
1948 ) . 34 For references and a review of the Fröhlich and Bardeen theories ...
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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 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