Introduction to Solid State Physics |
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Page 13
... plane perpendicular to it . The region of space which can be reached from O without crossing any of the planes then ... plane is determined by giving the coordinates of three atoms lying in the plane . If each of the atoms lies on a ...
... plane perpendicular to it . The region of space which can be reached from O without crossing any of the planes then ... plane is determined by giving the coordinates of three atoms lying in the plane . If each of the atoms lies on a ...
Page 21
... planes ( hkl ) must be parallel to the reflecting plane , and the diffraction maxima occur when the scattering direction may be derived from the incident direction by reflection in a lattice plane . If d ( hkl ) is the spacing between ...
... planes ( hkl ) must be parallel to the reflecting plane , and the diffraction maxima occur when the scattering direction may be derived from the incident direction by reflection in a lattice plane . If d ( hkl ) is the spacing between ...
Page 325
... plane of atoms on the upper half of the y axis . Atoms in the upper half - crystal P are compressed and those in the lower half Q are extended . This is defined as a positive dislocation ; if the extra plane is put in from below , the ...
... plane of atoms on the upper half of the y axis . Atoms in the upper half - crystal P are compressed and those in the lower half Q are extended . This is defined as a positive dislocation ; if the extra plane is put in from below , the ...
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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absorption alkali halides alkali metal alloy anisotropy antiferromagnetic approximation 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 entropy equation equilibrium experimental F-center factor Fermi ferroelectric ferromagnetic free electron frequency given heat capacity holes impurity interaction interstitial ionic crystals ionized lattice constant lattice points London low temperatures magnetic field magnetic moment molecules motion nearest neighbor normal observed orbital p-n junctions parallel paramagnetic particles perovskite phonons Phys physical plane polarizability polarization positive potassium chloride potential Proc quantum range order region resonance result room temperature scattering Seitz semiconductor Shockley shown in Fig single crystal sodium chloride solids specimen spin superconducting susceptibility symmetry Table theory thermal tion unit volume valence values vector velocity wave functions x-ray zero