Introduction to Solid State Physicsproblems after each chapter |
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Page 173
E = tion is neglected , the Onsager model gives ( 7.32 ) [ 1 + 3x + 3 ( 1 + ģx + x ? )
? ' ) , x = 4nNp2 / 3kT . It is easily seen that this expression , which is derived in
Appendix C , does not give a critical point . Further discussion of the problem ...
E = tion is neglected , the Onsager model gives ( 7.32 ) [ 1 + 3x + 3 ( 1 + ģx + x ? )
? ' ) , x = 4nNp2 / 3kT . It is easily seen that this expression , which is derived in
Appendix C , does not give a critical point . Further discussion of the problem ...
Page 520
18.13 current produced by the primary radiathe background photocurrent is tion
at 0.78 ev . It is known that 0.38 orresponds to produced by a constant light
required to free one trapped hole from level at 1.58 ( 0.78 ev ) . When a Mn atom
in ...
18.13 current produced by the primary radiathe background photocurrent is tion
at 0.78 ev . It is known that 0.38 orresponds to produced by a constant light
required to free one trapped hole from level at 1.58 ( 0.78 ev ) . When a Mn atom
in ...
Page 543
The broken vertical tion is the screw dislocation , sketched line which marks the
dislocation is in Figs . 19.7 and 19.8 . It marks a surrounded by strained material .
boundary between slipped and unslipped crystal . The boundary parallels the ...
The broken vertical tion is the screw dislocation , sketched line which marks the
dislocation is in Figs . 19.7 and 19.8 . It marks a surrounded by strained material .
boundary between slipped and unslipped crystal . The boundary parallels the ...
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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