Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Page 331
... levels as Landau levels perturbed by the Coulomb potential which is a small 2.4 Si ( Bi ) 2.0 BII ( 100 ) ELB term at high magnetic fields compared to the diamagnetic terms in the Hamil- tonian of the effective mass equation . In any ...
... levels as Landau levels perturbed by the Coulomb potential which is a small 2.4 Si ( Bi ) 2.0 BII ( 100 ) ELB term at high magnetic fields compared to the diamagnetic terms in the Hamil- tonian of the effective mass equation . In any ...
Page 410
... levels are completely filled , but the d - levels are either empty or partially filled , so the possibility of conduction in these levels exists . If they form a band of levels which is empty , then their behavior might be expected to ...
... levels are completely filled , but the d - levels are either empty or partially filled , so the possibility of conduction in these levels exists . If they form a band of levels which is empty , then their behavior might be expected to ...
Page 421
... levels . Equation ( 2 ) shows the formation of a conduction electron and a hole in the 3d levels . In ( 3 ) , a nickel 3d electron is excited to a 48 level , leaving behind a hole in the 3d levels . Equations ( 4 ) and ( 5 ) show how ...
... levels . Equation ( 2 ) shows the formation of a conduction electron and a hole in the 3d levels . In ( 3 ) , a nickel 3d electron is excited to a 48 level , leaving behind a hole in the 3d levels . Equations ( 4 ) and ( 5 ) show how ...
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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