Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Page 290
... coefficient analogous to that carried out for the absorption coefficient . Consequently approximate expressions for explaining the interband Faraday rotation were worked out . Other experiments involving interband magnetoreflection in ...
... coefficient analogous to that carried out for the absorption coefficient . Consequently approximate expressions for explaining the interband Faraday rotation were worked out . Other experiments involving interband magnetoreflection in ...
Page 294
... coefficient ( III.15 ) 2x : = 2e2 M ( 2μ 2 k = с √x m2 co h2 This expression for the attenuation coefficient holds quite well for transitions to bands where the effective mass is small but is questionable for transitions to levels with ...
... coefficient ( III.15 ) 2x : = 2e2 M ( 2μ 2 k = с √x m2 co h2 This expression for the attenuation coefficient holds quite well for transitions to bands where the effective mass is small but is questionable for transitions to levels with ...
Page 361
... coefficient for the { 111 } facets developed on the « core » of the crystal , to the distribution coefficient outside the core region , for several dif- ferent impurities was as follows : Element k ( core ) / k ( outside ) Р As Sb Bi Ga ...
... coefficient for the { 111 } facets developed on the « core » of the crystal , to the distribution coefficient outside the core region , for several dif- ferent impurities was as follows : Element k ( core ) / k ( outside ) Р As Sb Bi Ga ...
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Common terms and phrases
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