Introduction to Solid State Physicsproblems after each chapter |
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Page 357
DONOR IONIZATION ENERGIES OF PENTAVALENT IMPURITIES IN
GERMANIUM AND SILICON , IN EV P As Sb Si 0.045 0.019–0.056 0.039 Ge
0.0120 0.0127 0.0096 We note that the radius of the first Bohr orbit is increased
by the factor ...
DONOR IONIZATION ENERGIES OF PENTAVALENT IMPURITIES IN
GERMANIUM AND SILICON , IN EV P As Sb Si 0.045 0.019–0.056 0.039 Ge
0.0120 0.0127 0.0096 We note that the radius of the first Bohr orbit is increased
by the factor ...
Page 383
Thus , the development of the high - back - voltage germanium rectifier by S.
Benzer at Purdue Universtity in 1942 was an important step toward the ultimate
development of the transistor . We begin with a short section on the preparation
of ...
Thus , the development of the high - back - voltage germanium rectifier by S.
Benzer at Purdue Universtity in 1942 was an important step toward the ultimate
development of the transistor . We begin with a short section on the preparation
of ...
Page 384
If we can progressively pass a melted section along an otherwise solid
germanium rod the impurities will collect in the melted section . They will be
swept along and concentrated in one end of the rod . A short section of this end is
discarded ...
If we can progressively pass a melted section along an otherwise solid
germanium rod the impurities will collect in the melted section . They will be
swept along and concentrated in one end of the rod . A short section of this end is
discarded ...
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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