Introduction to Solid State Physicsproblems after each chapter |
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Page 88
There are nine stress components : Xă , Xy , X2 , Y. , Yu , Y. , Z2 , Zy , Zz . The capital letter indicates the direction of the force , and the subscript indicates the normal to the plane to which the force Xy is applied .
There are nine stress components : Xă , Xy , X2 , Y. , Yu , Y. , Z2 , Zy , Zz . The capital letter indicates the direction of the force , and the subscript indicates the normal to the plane to which the force Xy is applied .
Page 180
( a ) Show that the expression ( 7.14 ) applied to the first Bohr orbit of the hydrogen atom gives a an ' , where an is the Bohr radius . ( b ) Consider a semiclassical model of the ground state of the hydrogen atom in an electric field ...
( a ) Show that the expression ( 7.14 ) applied to the first Bohr orbit of the hydrogen atom gives a an ' , where an is the Bohr radius . ( b ) Consider a semiclassical model of the ground state of the hydrogen atom in an electric field ...
Page 299
We now consider in detail the motion of a hole in an applied electric field . We treat the one - dimensional example illustrated by Fig . 11.15 . Initially the band is filled except for the single vacant state F at the top of the band .
We now consider in detail the motion of a hole in an applied electric field . We treat the one - dimensional example illustrated by Fig . 11.15 . Initially the band is filled except for the single vacant state F at the top of the band .
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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