Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Page 88
... charge zero . It may happen that structure elements are ionized by the addition or removal of one or more electrons . In that case the effective charge of the centre is obviously no longer zero , but equal to the added or equal but ...
... charge zero . It may happen that structure elements are ionized by the addition or removal of one or more electrons . In that case the effective charge of the centre is obviously no longer zero , but equal to the added or equal but ...
Page 162
... charge ( valence ) as the M ( or X ) atom substituted by it . Therefore when , for instance in Fig . 41 in ranges III and IV the foreign atom is mainly present as FM , one may say that in this case those ranges correspond to a region of ...
... charge ( valence ) as the M ( or X ) atom substituted by it . Therefore when , for instance in Fig . 41 in ranges III and IV the foreign atom is mainly present as FM , one may say that in this case those ranges correspond to a region of ...
Page 430
... Charge - transfer complexes . We turn now to the second , and newer , major class of organic semicon- ductors , the charge - transfer complexes . These are intermolecular addition com- pounds formed by the combination of an electron ...
... Charge - transfer complexes . We turn now to the second , and newer , major class of organic semicon- ductors , the charge - transfer complexes . These are intermolecular addition com- pounds formed by the combination of an electron ...
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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