Introduction to Solid State PhysicsProblems after each chapter. |
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Page 17
... axes . One- , two- , three- , four- , and six - fold rotation axes are permissible , corresponding to rotations by 360 ° , 180 ° , 120 ° , 90 ° , and 60 ° . The rotation axes are denoted by the symbols 1 , 2 , 3 , 4 , and 6. The axes 2 ...
... axes . One- , two- , three- , four- , and six - fold rotation axes are permissible , corresponding to rotations by 360 ° , 180 ° , 120 ° , 90 ° , and 60 ° . The rotation axes are denoted by the symbols 1 , 2 , 3 , 4 , and 6. The axes 2 ...
Page 85
... axes a , b , c , the strain may be specified by the changes Aα , Aß , Ay ; Aa , Ab , Ac resulting from the deformation . This is a good physical specification of strain , but for non - orthogonal axes it leads to mathematical ...
... axes a , b , c , the strain may be specified by the changes Aα , Aß , Ay ; Aa , Ab , Ac resulting from the deformation . This is a good physical specification of strain , but for non - orthogonal axes it leads to mathematical ...
Page 86
... axes are Ezz , Ey , Ezz , respectively , to the first order . We define the strain components h + 90 ° 90 ° 90 ° f | fg | = h = 1 ( a ) h ( b ) g ' Fig . 4.1 . Coordinate axes for the description of the state of strain ; the orthogonal ...
... axes are Ezz , Ey , Ezz , respectively , to the first order . We define the strain components h + 90 ° 90 ° 90 ° f | fg | = h = 1 ( a ) h ( b ) g ' Fig . 4.1 . Coordinate axes for the description of the state of strain ; the orthogonal ...
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 region resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory tion transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero