Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Page 90
... imperfections , no interaction with the base crystal . After these introductory sections some physicochemical aspects in semi- conductors or isolators will be treated somewhat more closely . We will start with one - phase systems , that ...
... imperfections , no interaction with the base crystal . After these introductory sections some physicochemical aspects in semi- conductors or isolators will be treated somewhat more closely . We will start with one - phase systems , that ...
Page 93
... imperfections and the base crystal . The simple cases treated so far did not include interactions of imperfections with the base crystal . However very often these interactions actually take place . Three examples of this kind of ...
... imperfections and the base crystal . The simple cases treated so far did not include interactions of imperfections with the base crystal . However very often these interactions actually take place . Three examples of this kind of ...
Page 144
... imperfections for a given concentration of F ( [ FM ] tot = 4.1018 cm - 3 ) as a function of PM for the case of Fig . 40 . Figure 42 gives the situation for T = 0 ° K , assuming , as has been done in earlier examples , that , during ...
... imperfections for a given concentration of F ( [ FM ] tot = 4.1018 cm - 3 ) as a function of PM for the case of Fig . 40 . Figure 42 gives the situation for T = 0 ° K , assuming , as has been done in earlier examples , that , during ...
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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