Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Page 202
Lattice (phonon) scattering. Single phonon collisions (multiple phonon processes
are very unlikely and can be neglected) can be described cither by interaction
between electron and lattice waves or by collisions between particles, the
phonon ...
Lattice (phonon) scattering. Single phonon collisions (multiple phonon processes
are very unlikely and can be neglected) can be described cither by interaction
between electron and lattice waves or by collisions between particles, the
phonon ...
Page 510
Since the LA and LO modes are degenerate (see Dr. Cochran's lectures) at the
zone edge in the <100> directions we should expect the TO phonon as used
here to be the more energetic. This is also in accordance with the neutron
scattering ...
Since the LA and LO modes are degenerate (see Dr. Cochran's lectures) at the
zone edge in the <100> directions we should expect the TO phonon as used
here to be the more energetic. This is also in accordance with the neutron
scattering ...
Page 513
involving emission of a phonon, when hv > AE + Ev, and as (hv — AE+Ev)* for
transitions involving absorption of a phonon, when hv > AE — Ev, AE being as
usual the forbidden energy gap and Ev the phonon energy equal to hco(q). Here
q is ...
involving emission of a phonon, when hv > AE + Ev, and as (hv — AE+Ev)* for
transitions involving absorption of a phonon, when hv > AE — Ev, AE being as
usual the forbidden energy gap and Ev the phonon energy equal to hco(q). Here
q is ...
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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