Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Page 325
... Zeeman Effect . 1. Introduction . - The Zeeman effect in semiconductors has been considered both theoretically and experimentally for two general classes of problems : impurity levels and exciton transitions . Initial calculations of the ...
... Zeeman Effect . 1. Introduction . - The Zeeman effect in semiconductors has been considered both theoretically and experimentally for two general classes of problems : impurity levels and exciton transitions . Initial calculations of the ...
Page 326
... Zeeman effect . However , as the structure was developed , particularly in the case of the in- direct exciton transition , it became necessary to develop a phenomenological theory similar to that of the spin Hamiltonian for paramagnetic ...
... Zeeman effect . However , as the structure was developed , particularly in the case of the in- direct exciton transition , it became necessary to develop a phenomenological theory similar to that of the spin Hamiltonian for paramagnetic ...
Page 331
... Zeeman splitting Aε ( electron volt 10 ) 1.0 ( 110 ) m = 0.185 mo EIB 1.6 EIB ( 111 ) ELB 1.2 m * = 0.188 mo m * = 0.182 mo 0.8 m - 0.187 m 0.4 0.6 2x AE in units of eĥ H / 2m , c 20 0.2 90 0.2 2x 0.6 0 10 - 20 30 1.0 40 20 40 [ 100 ] 4 ...
... Zeeman splitting Aε ( electron volt 10 ) 1.0 ( 110 ) m = 0.185 mo EIB 1.6 EIB ( 111 ) ELB 1.2 m * = 0.188 mo m * = 0.182 mo 0.8 m - 0.187 m 0.4 0.6 2x AE in units of eĥ H / 2m , c 20 0.2 90 0.2 2x 0.6 0 10 - 20 30 1.0 40 20 40 [ 100 ] 4 ...
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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