Introduction to Solid State Physicsproblems after each chapter |
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Page 8
fi a ( a ) Square lattice lal = | bl ; y = 90 ° ( 6 ) Hexagonal lattice lal = Tbl ; y = 120 ° b म b . ( c ) Rectangular lattice lal # Ibl ; y = 90 ° ( d ) Centered rectangular lattice ; axes are shown for both the primitive cell and ...
fi a ( a ) Square lattice lal = | bl ; y = 90 ° ( 6 ) Hexagonal lattice lal = Tbl ; y = 120 ° b म b . ( c ) Rectangular lattice lal # Ibl ; y = 90 ° ( d ) Centered rectangular lattice ; axes are shown for both the primitive cell and ...
Page 26
In the triclinic system the single space lattice has a primitive ( P ) unit cell , with three axes of unequal lengths and unequal angles . The symmetry of the lattice is ī , all space lattices being invariant under inversion .
In the triclinic system the single space lattice has a primitive ( P ) unit cell , with three axes of unequal lengths and unequal angles . The symmetry of the lattice is ī , all space lattices being invariant under inversion .
Page 51
As an example we show that a foc lattice has as its reciprocal a bcc lattice . In the direct fcc lattice the distance between lattice planes in each cube edge direction is a / 2 , where a is the lattice constant ; thus there are points ...
As an example we show that a foc lattice has as its reciprocal a bcc lattice . In the direct fcc lattice the distance between lattice planes in each cube edge direction is a / 2 , where a is the lattice constant ; thus there are points ...
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic magnetic field mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone