Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Page 199
If /„ is the distribution function in zero field and / the disturbed distribution function
the equivalent of the equation of motion, eq. (2.1), is the Boltzmann equation
written in the form Of the two approaches the equation of motion gives a simpler ...
If /„ is the distribution function in zero field and / the disturbed distribution function
the equivalent of the equation of motion, eq. (2.1), is the Boltzmann equation
written in the form Of the two approaches the equation of motion gives a simpler ...
Page 243
In general, this is not so; the equations of motion are more complicated and must
be handled by means of a Boltzmann equation or by integrals which will be
derived later. 21. Conductivity of holes and electrons. - Since we are ultimately ...
In general, this is not so; the equations of motion are more complicated and must
be handled by means of a Boltzmann equation or by integrals which will be
derived later. 21. Conductivity of holes and electrons. - Since we are ultimately ...
Page 480
I shall begin by developing by pc curbation theory from the one-electron
Schrodinger equation an expressir.i for the effective mass at a band edge. This
will give us some feel for what properties of the solid govern the effective mass
and show ...
I shall begin by developing by pc curbation theory from the one-electron
Schrodinger equation an expressir.i for the effective mass at a band edge. This
will give us some feel for what properties of the solid govern the effective mass
and show ...
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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