Introduction to Solid State Physicsproblems after each chapter |
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Page 70
The hydrogen bond is an important interaction between H20 molecules and is
responsible , together with the electrostatic attraction of the electric dipole
moments , for the striking physical properties of water and ice . The hydrogen
bond ...
The hydrogen bond is an important interaction between H20 molecules and is
responsible , together with the electrostatic attraction of the electric dipole
moments , for the striking physical properties of water and ice . The hydrogen
bond ...
Page 189
The theory given now assumes implicitly that the transition is a second order
transition , but the physical ideas involved can be carried over in part to a first
order transition . ' J. C. Slater , Phys . Rev. 78 , 748 ( 1950 ) . We may rewrite (
7.10 ) in ...
The theory given now assumes implicitly that the transition is a second order
transition , but the physical ideas involved can be carried over in part to a first
order transition . ' J. C. Slater , Phys . Rev. 78 , 748 ( 1950 ) . We may rewrite (
7.10 ) in ...
Page 291
The change Aplat in the lattice momentum resulting from the change of state of
the electron may be derived by an elementary physical consideration . We are
familiar with the circumstance that an x - ray photon suffering Bragg reflection
from a ...
The change Aplat in the lattice momentum resulting from the change of state of
the electron may be derived by an elementary physical consideration . We are
familiar with the circumstance that an x - ray photon suffering Bragg reflection
from a ...
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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