Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Page 65
... assumed , so that R was determined by two parameters , for which in an earlier section we used a and B. The elements of the matrix T were assumed to be proportional to those of R since the elastic constants then depend only on a and ẞ ...
... assumed , so that R was determined by two parameters , for which in an earlier section we used a and B. The elements of the matrix T were assumed to be proportional to those of R since the elastic constants then depend only on a and ẞ ...
Page 139
... assumed that the constituents M and X of the solid phase interact with the vapour phase in such a way that their thermodynamic potential is determined by the partial pressures of the constituents M and X. The foreign atom F however ...
... assumed that the constituents M and X of the solid phase interact with the vapour phase in such a way that their thermodynamic potential is determined by the partial pressures of the constituents M and X. The foreign atom F however ...
Page 391
... assumed that equilibrium between the two kinds of sites was achieved , and this appeared to be justified by ... assumption of equilibrium means that the chemical potentials on the two kinds of sites are equal , i.e. , ( 11 ) MD = Ма ...
... assumed that equilibrium between the two kinds of sites was achieved , and this appeared to be justified by ... assumption of equilibrium means that the chemical potentials on the two kinds of sites are equal , i.e. , ( 11 ) MD = Ма ...
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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