Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Page 82
... constant , the use of G is extremely useful for questions like this . It has been shown ( Section 1 ) that for such a closed system , under constant pressure and constant temperature G has to be a minimum : ( 59 ) ( dG ) p.r.n ( MM ) .n ...
... constant , the use of G is extremely useful for questions like this . It has been shown ( Section 1 ) that for such a closed system , under constant pressure and constant temperature G has to be a minimum : ( 59 ) ( dG ) p.r.n ( MM ) .n ...
Page 271
... constant for the case of transverse propagation , with the electric field parallel to the magnetic field . Noting the σ22 = σo we obtain , for the parallel solution , ( II.13 ) r2 —— - ωδεμα + ίωμ , σο In an analogous manner one can ...
... constant for the case of transverse propagation , with the electric field parallel to the magnetic field . Noting the σ22 = σo we obtain , for the parallel solution , ( II.13 ) r2 —— - ωδεμα + ίωμ , σο In an analogous manner one can ...
Page 363
... constant as the crystal is pulled , the supply of material being continuously replenished by the large reservoir . The most generally useful means of arriving at a uniform impurity distri- bution is by « < zone - leveling » . Consider ...
... constant as the crystal is pulled , the supply of material being continuously replenished by the large reservoir . The most generally useful means of arriving at a uniform impurity distri- bution is by « < zone - leveling » . Consider ...
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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