Introduction to Solid State Physics |
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Page 17
... possible space groups . A full discussion of space groups is not possible in the space available here . We shall not require knowledge of the theory of space groups in order to understand the crystal structures explicitly discussed in ...
... possible space groups . A full discussion of space groups is not possible in the space available here . We shall not require knowledge of the theory of space groups in order to understand the crystal structures explicitly discussed in ...
Page 33
... possible to write down the successive terms by a casual inspection , nor is it possible to sum the series conveniently . It is important so to arrange the terms in the series that the contributions from the positive and negative terms ...
... possible to write down the successive terms by a casual inspection , nor is it possible to sum the series conveniently . It is important so to arrange the terms in the series that the contributions from the positive and negative terms ...
Page 104
... possible to determine the position of hydrogen atoms in a crystal by using x - rays , because of the low scatter- ing power of hydrogen . Neutron diffraction is a possible tool , especially if deuterium is substituted for hydrogen . The ...
... possible to determine the position of hydrogen atoms in a crystal by using x - rays , because of the low scatter- ing power of hydrogen . Neutron diffraction is a possible tool , especially if deuterium is substituted for hydrogen . The ...
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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absorption alkali alloy anisotropy antiferromagnetic approximately atoms axes axis Bardeen barium titanate boundary calculated charge coefficient conduction band cube Curie point Debye density diamagnetic dielectric constant diffraction diffusion dipole direction discussed dislocation displacement domains effect elastic electric field energy entropy equation equilibrium experimental F-centers factor Fermi ferroelectric ferromagnetic free electron frequency given heat capacity holes impurity interaction ionic crystals ionized ions lattice constant lattice points London low temperatures magnetic field magnetic moment metals molecules motion nearest neighbor normal observed optical orbital parallel paramagnetic particles perovskite phonons Phys physical plane polarizability polarization positive potassium potassium chloride potential Proc quantum resonance result room temperature scattering Seitz shear Shockley shown in Fig single crystal sodium chloride solids specimen spin strain stress superconducting surface susceptibility symmetry Table theory thermal tion transition unit volume vacancy valence values vector velocity wave functions x-ray zero