Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Results 1-3 of 61
Page 383
... samples were heated to successively higher tem- peratures and allowed to reach equilibrium . The mobilities after these heat treatments are shown in Fig . IV.1 for two pairs of samples , representing a control and a Li - containing sample ...
... samples were heated to successively higher tem- peratures and allowed to reach equilibrium . The mobilities after these heat treatments are shown in Fig . IV.1 for two pairs of samples , representing a control and a Li - containing sample ...
Page 401
... samples containing few disloca- tions , and samples with a large number of dislocations , the latter showing much faster precipitation rates . These results were interpreted as indicating that the precipitation nuclei were , initially ...
... samples containing few disloca- tions , and samples with a large number of dislocations , the latter showing much faster precipitation rates . These results were interpreted as indicating that the precipitation nuclei were , initially ...
Page 421
... samples . From eqs . ( 1 ) to ( 5 ) it can be seen that the total conductivity of NiO might involve three parallel ... samples studied , in pure NiO samples the hole conduction in the oxygen 2p band would be expected to dominate the ...
... samples . From eqs . ( 1 ) to ( 5 ) it can be seen that the total conductivity of NiO might involve three parallel ... samples studied , in pure NiO samples the hole conduction in the oxygen 2p band would be expected to dominate the ...
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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