Introduction to Solid State PhysicsProblems after each chapter. |
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Page 9
... Hexagonal 60 ° rhombus a = b , b , γ === = Y 90 ° Square 4 , 4mm 120 ° Hexagonal 3 , 3m , 6 , 6mm TWO - DIMENSIONAL SPACE GROUPS We remarked earlier in connection with Fig . 1.1 that a crystal struc- ture is formed by associating with ...
... Hexagonal 60 ° rhombus a = b , b , γ === = Y 90 ° Square 4 , 4mm 120 ° Hexagonal 3 , 3m , 6 , 6mm TWO - DIMENSIONAL SPACE GROUPS We remarked earlier in connection with Fig . 1.1 that a crystal struc- ture is formed by associating with ...
Page 35
... hexagonal space lattice one often uses hexagonal indices with the four axes a1 , a2 , aз , 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 number ...
... hexagonal space lattice one often uses hexagonal indices with the four axes a1 , a2 , aз , 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 number ...
Page 42
... Hexagonal close - packed Diamond # 22 / 6 ( = 0.74 ) # 32 / 16 ( = 0.34 ) 1 We may note that by experiment [ O. K. Rice , J. Chem . Phys . 12 , 1 ( 1944 ) ] it is found that the volume of an arrangement of spheres packed at random into ...
... Hexagonal close - packed Diamond # 22 / 6 ( = 0.74 ) # 32 / 16 ( = 0.34 ) 1 We may note that by experiment [ O. K. Rice , J. Chem . Phys . 12 , 1 ( 1944 ) ] it is found that the volume of an arrangement of spheres packed at random into ...
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 levels 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