Introduction to Solid State Physicsproblems after each chapter |
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General References Crystallography F . C . Phillips , An introduction to
crystallography , Longmans , London , 1946 . M . J . Buerger , Elementary
crystallography , John Wiley & Sons , New York , 1956 . Atomic physics
background Max Born ...
General References Crystallography F . C . Phillips , An introduction to
crystallography , Longmans , London , 1946 . M . J . Buerger , Elementary
crystallography , John Wiley & Sons , New York , 1956 . Atomic physics
background Max Born ...
Page 74
3 ) , a = ( + ) pij - ? , where now , if we take the reference ion as a negative charge
, the plus sign will be used for positive ions and the minus sign for negative ions .
An equivalent definition is - " ( + ) ( 3 . 6 ) " ' ; where r ; is the distance of the jth ...
3 ) , a = ( + ) pij - ? , where now , if we take the reference ion as a negative charge
, the plus sign will be used for positive ions and the minus sign for negative ions .
An equivalent definition is - " ( + ) ( 3 . 6 ) " ' ; where r ; is the distance of the jth ...
Page 573
The potential to at the reference ion point i due to the central Gaussian
distribution is ( A . 10 ) Aar2 dr ) ( / r ) = 2qi ( n / a ) ” , and so ( A . 11 ) Vii ) = 1 - %
e - G2 / 49 – 2qi ( n / a ) " . The potential ¥2 is to be evaluated at the reference
point , and it ...
The potential to at the reference ion point i due to the central Gaussian
distribution is ( A . 10 ) Aar2 dr ) ( / r ) = 2qi ( n / a ) ” , and so ( A . 11 ) Vii ) = 1 - %
e - G2 / 49 – 2qi ( n / a ) " . The potential ¥2 is to be evaluated at the reference
point , and it ...
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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 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