Introduction to Solid State Physicsproblems after each chapter |
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Page 8
b F A a ( a ) Square lattice lal = b ; y = 90 ° ( b ) Hexagonal lattice lal = ibl ; y = 120
° b a a ( c ) Rectangular lattice ial # Ibl ; y = 90 ° ( d ) Centered rectangular lattice ;
axes are shown for both the primitive cell and for the rectangular unit cell , for ...
b F A a ( a ) Square lattice lal = b ; y = 90 ° ( b ) Hexagonal lattice lal = ibl ; y = 120
° b a a ( c ) Rectangular lattice ial # Ibl ; y = 90 ° ( d ) Centered rectangular lattice ;
axes are shown for both the primitive cell and for the rectangular unit cell , for ...
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 in variant under inversion . In the monoclinic system ...
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 in variant under inversion . In the monoclinic system ...
Page 51
As an example we show that a fce lattice has as its reciprocal a bec lattice . In the
direct foc lattice the distance between lattice planes in each cube edge direction
is a / 2 , where a is the lattice constant ; thus there are points in the reciprocal ...
As an example we show that a fce lattice has as its reciprocal a bec lattice . In the
direct foc lattice the distance between lattice planes in each cube edge direction
is a / 2 , where a is the lattice constant ; thus there are points in the reciprocal ...
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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 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