Introduction to Solid State Physicsproblems after each chapter |
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Page 14
mm 4 4mm 4mm 3 3m oo OS No. 15 p3lm 3m Hexagonal. No. 9 c2mm
Rectangular 88 No. 10 p4 Square No. 11 p4mm Square Square No. 12 p4gm
Hexagonal No. 13 p3 o Hexagonal 14 THE DESCRIPTION OF CRYSTAL
STRUCTURES.
mm 4 4mm 4mm 3 3m oo OS No. 15 p3lm 3m Hexagonal. No. 9 c2mm
Rectangular 88 No. 10 p4 Square No. 11 p4mm Square Square No. 12 p4gm
Hexagonal No. 13 p3 o Hexagonal 14 THE DESCRIPTION OF CRYSTAL
STRUCTURES.
Page 35
In the hexagonal space lattice one often uses hexagonal indices with the four
axes Q1 , Q2 , A3 , 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 Q1 , Q2 , A3 , 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
... 134 , 257 , 293 electrons , 242 internal motion , 137 solids , 121
superconductors , 455 , 463 table for metals , 259 Heat conductivity , see Thermal
conductivity Hexagonal close - packed structure , 35 Hexagonal lattice , 8
Hexagonal system ...
... 134 , 257 , 293 electrons , 242 internal motion , 137 solids , 121
superconductors , 455 , 463 table for metals , 259 Heat conductivity , see Thermal
conductivity Hexagonal close - packed structure , 35 Hexagonal lattice , 8
Hexagonal system ...
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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