Introduction to Solid State Physicsproblems after each chapter |
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Page 173
It is not possible to determine the position of hydrogen atoms in a crystal by using
X - rays , because of the low scattering power of hydrogen . Neutron diffraction is
a possible tool , especially if deuterium is substituted for hydrogen .
It is not possible to determine the position of hydrogen atoms in a crystal by using
X - rays , because of the low scattering power of hydrogen . Neutron diffraction is
a possible tool , especially if deuterium is substituted for hydrogen .
Page 400
of e 2.72 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 ...
of e 2.72 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 ...
Page 490
KIRKENDALL EFFECT A distinction between the interchange mechanism on the
one hand and interstitial and vacancy mechanisms on the other hand is offered
by the Kirkendall effect , 13 Fig . 17.11 . Suppose that it is possible ...
KIRKENDALL EFFECT A distinction between the interchange mechanism on the
one hand and interstitial and vacancy mechanisms on the other hand is offered
by the Kirkendall effect , 13 Fig . 17.11 . Suppose that it is possible ...
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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