Introduction to Solid State Physicsproblems after each chapter |
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Page 395
In fact p - n junctions have as good rectification curves as it is possible to have for
simple structures using carriers of one electron charge . POINT CONTACT
TRANSISTORS The point contact transistor , discovered by Bardeen and Brattain
...
In fact p - n junctions have as good rectification curves as it is possible to have for
simple structures using carriers of one electron charge . POINT CONTACT
TRANSISTORS The point contact transistor , discovered by Bardeen and Brattain
...
Page 400
72 for each increase of kT / e in the forward voltage across the emitter base
junction and this is the highest sensitivity possible for a structure with singly
charged current carriers controlled by a potential hill . The properties of p - n
junctions ...
72 for each increase of kT / e in the forward voltage across the emitter base
junction and this is the highest sensitivity possible for a structure with singly
charged current carriers controlled by a potential hill . The properties of p - n
junctions ...
Page 490
Suppose that it is possible to regard the lattice framework of a crystal as a rigid
frame of cells between which the atoms jump ; on the interchange mechanism ,
pairs of atoms change places simultaneously , and there is no displacement of
the ...
Suppose that it is possible to regard the lattice framework of a crystal as a rigid
frame of cells between which the atoms jump ; on the interchange mechanism ,
pairs of atoms change places simultaneously , and there is no displacement of
the ...
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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