Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Page 267
... effect could also have been called the Cotton - Mouton effect . However , TEITLER and PALIK , who first observed it in semiconductors , chose to call it the Voigt effect . Interband effects in a magnetic field were first found in ...
... effect could also have been called the Cotton - Mouton effect . However , TEITLER and PALIK , who first observed it in semiconductors , chose to call it the Voigt effect . Interband effects in a magnetic field were first found in ...
Page 284
... Voigt effect is one to two orders of magnitude smaller than the Faraday effect . Nevertheless it is still measurable ; a typical value of rotation would be 10 ° / mm . The Voigt effect has been measured in n - type indium arsenide by ...
... Voigt effect is one to two orders of magnitude smaller than the Faraday effect . Nevertheless it is still measurable ; a typical value of rotation would be 10 ° / mm . The Voigt effect has been measured in n - type indium arsenide by ...
Page 324
... Voigt - effect phase shift to exceed the Faraday rotation . Hence , at low temperatures particularly ( which would tend to make 7 larger ) , the oscillatory Voigt effect can be readily observed . The two sets of measurements on Aẞ and ...
... Voigt - effect phase shift to exceed the Faraday rotation . Hence , at low temperatures particularly ( which would tend to make 7 larger ) , the oscillatory Voigt effect can be readily observed . The two sets of measurements on Aẞ and ...
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absorption acceptor approximation band edge band structure Brillouin zone calculated carrier Chem coefficient compound concentration conduction band constant corresponding crystal cyclotron resonance density diffusion direction 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 K,PM K₁ lattice levels linear liquid magnetic field matrix measurements melt mobility momentum N₁ obtained optical p-type phase phonon Phys potential pressure quantum range reciprocal lattice region Rendiconti S.I.F. samples scattering semiconductors shown in Fig solid spin-orbit structure elements symmetry temperature tensor theory thermodynamic potentials transition transverse valence band Voigt effect wave functions wave vector Zeeman effect zero zone