Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Page 227
The observation consists of the generation of a transverse electric field in a bar of
N germanium when a large electric field is applied longitudinally, provided the
latter direction does not coincide with a crystal symmetry direction. Assume that a
...
The observation consists of the generation of a transverse electric field in a bar of
N germanium when a large electric field is applied longitudinally, provided the
latter direction does not coincide with a crystal symmetry direction. Assume that a
...
Page 437
This sample may (or may not) form a part of an electric and heat circuit with an
ideal metal connected to its ends in the ... Let us direct the magnetic field along
the positive z axis and consider electric fields, thermal gradients and electric and
...
This sample may (or may not) form a part of an electric and heat circuit with an
ideal metal connected to its ends in the ... Let us direct the magnetic field along
the positive z axis and consider electric fields, thermal gradients and electric and
...
Page 451
Instead of tending to zero, as in the case of a single band, N± tends to a value
independent of the magnetic field, which means that ... The magnetic field
deflects electrons and holes in opposite directions creating thus a transverse
electric field.
Instead of tending to zero, as in the case of a single band, N± tends to a value
independent of the magnetic field, which means that ... The magnetic field
deflects electrons and holes in opposite directions creating thus a transverse
electric field.
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absorption acceptor approximation assumed band edge band structure Brillouin zone calculated carrier centre charge Chem coefficient components compound concentration conduction band consider constant corresponding crystal curves cyclotron resonance degenerate density diffusion direct transition discussed donor doping effective mass electric field energy gap energy surfaces equation equilibrium example exciton experimental expression Faraday rotation foreign atoms free electron frequency germanium given hence holes imperfections impurity indium antimonide InSb interaction interband ionization ions Journ lattice levels linear liquid magnetic field matrix measurements melt mobility momentum obtained optical p-type phonon Phys potential pressure quantum range reciprocal lattice region samples scattering semiconductors shown in Fig spherical spin spin-orbit structure elements symmetry tensor theory thermodynamic thermodynamic potentials tion transverse valence band valley Voigt effect wave functions wave vector Zeeman effect zero zone