Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Page 96
... germanium . As will be clear the self - diffusion of germanium will be proportional to the total concentration of the vacant germanium sites : [ Vge ] + [ V ́e ] · Ge . As has been said already [ Vee ] is constant . From ( 96 ) and ...
... germanium . As will be clear the self - diffusion of germanium will be proportional to the total concentration of the vacant germanium sites : [ Vge ] + [ V ́e ] · Ge . As has been said already [ Vee ] is constant . From ( 96 ) and ...
Page 204
... germanium , shear forces can change the relative energy of the valleys and so make the conduc- tivity anisotropic . To a first order , scattering by transverse acoustic modes will involve a different deformation potential but will ...
... germanium , shear forces can change the relative energy of the valleys and so make the conduc- tivity anisotropic . To a first order , scattering by transverse acoustic modes will involve a different deformation potential but will ...
Page 253
and C for both germanium and silicon . For example , for germanium , we find 111 ML A + B + C2 1 4 = 0.154 , Mo for the heavy hole with the magnetic field in the [ 111 ] direction 111 MH Mo 1 - A - V B2 + 0.54 , 4 for the heavy hole and ...
and C for both germanium and silicon . For example , for germanium , we find 111 ML A + B + C2 1 4 = 0.154 , Mo for the heavy hole with the magnetic field in the [ 111 ] direction 111 MH Mo 1 - A - V B2 + 0.54 , 4 for the heavy hole 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