Introduction to Solid State Physicsproblems after each chapter |
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Page 157
The polarization is defined as the dipole moment per unit volume , the dipole
moment of the specimen as a whole being defined as P = Seifi . The sum is
extended over all charges in the system ; on the supposition that the system is
neutral the ...
The polarization is defined as the dipole moment per unit volume , the dipole
moment of the specimen as a whole being defined as P = Seifi . The sum is
extended over all charges in the system ; on the supposition that the system is
neutral the ...
Page 380
Conductivity of germanium specimens originally n - and p - type as a function of
the integrated deuteron flux to which the ... The variation of conductivity of the
specimen initially n - type is attributed to the production of acceptors which
gradually ...
Conductivity of germanium specimens originally n - and p - type as a function of
the integrated deuteron flux to which the ... The variation of conductivity of the
specimen initially n - type is attributed to the production of acceptors which
gradually ...
Page 414
15 FERROMAGNETIC DOMAINS17 At temperatures well below the Curie point
the electronic magnetic moments of a ferromagnetic specimen are essentially all
lined up , when regarded on a microscopic scale . Yet , looking at a specimen as
...
15 FERROMAGNETIC DOMAINS17 At temperatures well below the Curie point
the electronic magnetic moments of a ferromagnetic specimen are essentially all
lined up , when regarded on a microscopic scale . Yet , looking at a specimen as
...
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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 neighbor 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