Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Page 78
total free energy of this four-component system may be written as: (46) 0 = NApA
+ Na/iB + NCiuc + NDflD where (23) do (47) ^A^\3JT) ' etc., and where the
quantities [iA, fiB etc. are called the thermodynamic potentials of the components
A, B, ...
total free energy of this four-component system may be written as: (46) 0 = NApA
+ Na/iB + NCiuc + NDflD where (23) do (47) ^A^\3JT) ' etc., and where the
quantities [iA, fiB etc. are called the thermodynamic potentials of the components
A, B, ...
Page 126
Now in every phase for n components (n — 1) mole fractions are necessary in
order to completely describe its composition. Therefore in order to describe the
system completely r(n — 1) + 2 data are needed, the term 2 originating from the ...
Now in every phase for n components (n — 1) mole fractions are necessary in
order to completely describe its composition. Therefore in order to describe the
system completely r(n — 1) + 2 data are needed, the term 2 originating from the ...
Page 516
For the i'th valley, the variation 8EW of each such level is presumed to be the
same linear homogeneous function of the strain components: Here c is the strain
tensor with components e„. Since &Em must be a scalar, the set of coefficients Sr,
...
For the i'th valley, the variation 8EW of each such level is presumed to be the
same linear homogeneous function of the strain components: Here c is the strain
tensor with components e„. Since &Em must be a scalar, the set of coefficients Sr,
...
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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