Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Page 98
These thermodynamic potentials then may be fixed by means of the
concentration of the particular atoms in a second phase (mostly liquid or gaseous
) in equilibrium with the solid under consideration. In general one can say that in
these cases ...
These thermodynamic potentials then may be fixed by means of the
concentration of the particular atoms in a second phase (mostly liquid or gaseous
) in equilibrium with the solid under consideration. In general one can say that in
these cases ...
Page 129
29 one sees the co-existing liquid-vapour phases, A2C2 and A2B2 with
compositions very rich in M and at the right hand side the co-existing liquid-
vapour phases H2G2 and H2K2 with compo- sof/tf M+ solid MX solid M + vapour
solid MX+1 ...
29 one sees the co-existing liquid-vapour phases, A2C2 and A2B2 with
compositions very rich in M and at the right hand side the co-existing liquid-
vapour phases H2G2 and H2K2 with compo- sof/tf M+ solid MX solid M + vapour
solid MX+1 ...
Page 342
There are a number of factors which determine the liquid-solid interface, the
temperature of which must be at the melting point of the growing crystal of course.
The liquid is maintained at a temperature above this point by means of an
external ...
There are a number of factors which determine the liquid-solid interface, the
temperature of which must be at the melting point of the growing crystal of course.
The liquid is maintained at a temperature above this point by means of an
external ...
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absorption acceptor approximation assumed band edge band structure Brillouin zone calculated carrier centre charge Chem coefficient components compound concentration conduction band consider constant corresponding crystal curves cyclotron resonance degenerate density diffusion direct transition discussed 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 lattice levels linear liquid magnetic field matrix measurements melt mobility momentum obtained optical p-type phonon Phys potential pressure quantum range reciprocal lattice region samples scattering semiconductors shown in Fig spherical spin spin-orbit structure elements symmetry tensor theory thermodynamic thermodynamic potentials tion transverse valence band valley Voigt effect wave functions wave vector Zeeman effect zero zone