Introduction to Solid State Physicsproblems after each chapter |
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Page 225
The Electromagnet Specimen Tor - f supply and circuit for measuring losses H , (
static ) r - f coil Fig . 9 . 7 . Schematic ... The r - f power absorbed in the specimen
is determined by electrical measurements , as by measuring the of the coil .
The Electromagnet Specimen Tor - f supply and circuit for measuring losses H , (
static ) r - f coil Fig . 9 . 7 . Schematic ... The r - f power absorbed in the specimen
is determined by electrical measurements , as by measuring the of the coil .
Page 456
In d - c measurements the resistivity in the superconducting state is zero . ... that
of the normal state ; that is , no change in the resistivity , as measured by the
reflection coefficient , is observed on passing through the critical magnetic field .
In d - c measurements the resistivity in the superconducting state is zero . ... that
of the normal state ; that is , no change in the resistivity , as measured by the
reflection coefficient , is observed on passing through the critical magnetic field .
Page 469
Curve Sh from magnetic susceptibility measurements on colloidal mercury ( from
D . Shoenberg , Nature 143 , 434 ( 1939 ) ] ; curves I and II from high - frequency
resistance measurements ( from A . B . Pippard , Proc . Roy . Soc . ( London ) ...
Curve Sh from magnetic susceptibility measurements on colloidal mercury ( from
D . Shoenberg , Nature 143 , 434 ( 1939 ) ] ; curves I and II from high - frequency
resistance measurements ( from A . B . Pippard , Proc . Roy . Soc . ( London ) ...
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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