Introduction to Solid State PhysicsProblems after each chapter. |
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Page 3
... cell , which is a type of unit cell . We shall later discuss unit cells in detail , but it will suffice now to state that the crystal translation operations applied to a unit cell will cover all points of the plane . A unit cell which ...
... cell , which is a type of unit cell . We shall later discuss unit cells in detail , but it will suffice now to state that the crystal translation operations applied to a unit cell will cover all points of the plane . A unit cell which ...
Page 26
... cells are not always primitive , as sometimes a multiply primitive cell has a closer connection with the symmetry elements than has a primitive cell . In the triclinic system the single space lattice has a primitive ( P ) unit cell ...
... cells are not always primitive , as sometimes a multiply primitive cell has a closer connection with the symmetry elements than has a primitive cell . In the triclinic system the single space lattice has a primitive ( P ) unit cell ...
Page 252
... cell by the set of numbers nr , ny , nz , m2 . The occupation number of a cell is either 0 or 1. We consider now a set of g , cells having approximately the same energy E as given by ( 10.37 ) , and we let the number of electrons in the ...
... cell by the set of numbers nr , ny , nz , m2 . The occupation number of a cell is either 0 or 1. We consider now a set of g , cells having approximately the same energy E as given by ( 10.37 ) , and we let the number of electrons in the ...
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS 85 | 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 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