Introduction to Solid State Physicsproblems after each chapter |
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Page 15
Charles Kittel. 1 No. 12 p4gm 4mm Square o No. 13 P3 3 Hexagonal O MA No. 14 p3ml 3m Hexagonal OO No. 15 p3lm 3m Hexagonal No. 16 p6 6 Hexagonal TWO - DIMENSIONAL CRYSTALS 15.
Charles Kittel. 1 No. 12 p4gm 4mm Square o No. 13 P3 3 Hexagonal O MA No. 14 p3ml 3m Hexagonal OO No. 15 p3lm 3m Hexagonal No. 16 p6 6 Hexagonal TWO - DIMENSIONAL CRYSTALS 15.
Page 35
In the hexagonal space lattice one often uses hexagonal indices with the four axes ai , 42 , 43 , C , as shown in Fig . 1.15 . In this notation the c axis is the ( 0001 ] direction . SIMPLE CRYSTAL STRUCTURES We discuss briefly a small ...
In the hexagonal space lattice one often uses hexagonal indices with the four axes ai , 42 , 43 , C , as shown in Fig . 1.15 . In this notation the c axis is the ( 0001 ] direction . SIMPLE CRYSTAL STRUCTURES We discuss briefly a small ...
Page 612
ductivity Hexagonal close - packed structure , 35 Hexagonal lattice , 8 Hexagonal system , 24 , 29 Hole injection , 369 Holes , 298 Holohedral point groups , 9 Hume - Rothery rules , 322 Hund rules , 217 Hydrogen bonds , 64 , 69 ...
ductivity Hexagonal close - packed structure , 35 Hexagonal lattice , 8 Hexagonal system , 24 , 29 Hole injection , 369 Holes , 298 Holohedral point groups , 9 Hume - Rothery rules , 322 Hund rules , 217 Hydrogen bonds , 64 , 69 ...
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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 present 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