Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Page 134
... corresponding to this equilibrium is given on the p , T projection by the line . efR . It has been said already that for these equilibria the pressure is a minimum in a p , x cut . Therefore the lines efR or E , E2 , E3 , E 、, called ...
... corresponding to this equilibrium is given on the p , T projection by the line . efR . It has been said already that for these equilibria the pressure is a minimum in a p , x cut . Therefore the lines efR or E , E2 , E3 , E 、, called ...
Page 165
... corresponding to those of the regions [ FM ] = n in Fig . 41 , 43 , 49. It must be said however that often a careful consideration of the possibility of incorporation according for instance to the region [ ( FV ) ' ] = p in Fig . 54 or ...
... corresponding to those of the regions [ FM ] = n in Fig . 41 , 43 , 49. It must be said however that often a careful consideration of the possibility of incorporation according for instance to the region [ ( FV ) ' ] = p in Fig . 54 or ...
Page 303
... correspond to the An = 0 transition which is split due to spin - orbit effects . From the experimental results the calculated effective g - factor of the electron corresponding to the energy split- ting is equal to 54. This anomalous g ...
... correspond to the An = 0 transition which is split due to spin - orbit effects . From the experimental results the calculated effective g - factor of the electron corresponding to the energy split- ting is equal to 54. This anomalous g ...
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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