Introduction to Solid State Physicsproblems after each chapter |
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Page 46
It should be emphasized that the Bragg equation results from the fundamental
periodicity of the structure , and the equation does not refer to the actual
composition or arrangement of the atoms associated with the reflecting planes .
The latter ...
It should be emphasized that the Bragg equation results from the fundamental
periodicity of the structure , and the equation does not refer to the actual
composition or arrangement of the atoms associated with the reflecting planes .
The latter ...
Page 245
In this equation 22 22 22 əx2 + ay2 + ozzi h = h / 27 ; and E is the total energy ,
which is constant . The function y is the wave function or eigenfunction , and has
the significance that , when properly normalized , y * y dxdydz is the probability of
...
In this equation 22 22 22 əx2 + ay2 + ozzi h = h / 27 ; and E is the total energy ,
which is constant . The function y is the wave function or eigenfunction , and has
the significance that , when properly normalized , y * y dxdydz is the probability of
...
Page 613
... superconductivity , 456 Local fields , perovskite structure , 192 London
equations , superconductivity , 464 Long range ... 215 Langevin - Debye
equation , 171 Langevin diamagnetism , equation , 207 Langevin function , 170 ,
213 Langevin ...
... superconductivity , 456 Local fields , perovskite structure , 192 London
equations , superconductivity , 464 Long range ... 215 Langevin - Debye
equation , 171 Langevin diamagnetism , equation , 207 Langevin function , 170 ,
213 Langevin ...
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
Copyright | |
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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 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