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THz instability by streaming carriers in high mobility solid-state plasmas
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10.1063/1.1937421
/content/aip/journal/pop/12/7/10.1063/1.1937421
http://aip.metastore.ingenta.com/content/aip/journal/pop/12/7/10.1063/1.1937421
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Graphic illustration of the dispersion relation solutions; real roots exist at the intersections (circles) of the beam plasma wave (solid) and the lattice phonon branch (dashed) curves (a) , four real roots (b) and (c) , two real roots. The other two roots are complex (instability) if the encircled branches do not intersect. All frequencies normalized to .

Image of FIG. 2.
FIG. 2.

Dispersion relation of the unstable, longitudinal (ES), beam plasmon/phonon polaron branch (a) (b) vs for various values of .

Image of FIG. 3.
FIG. 3.

Graphic illustration of the roots, at the intersections of the beam plasma wave (solid) and the lattice phonon branch (dashed) curves, for the sixth order electromagnetic (transverse) mode dispersion relation. There are always four real solutions—the two remaining roots are always complex (instability).

Image of FIG. 4.
FIG. 4.

Dispersion relation of the unstable, transverse (EM), beam plasmon/phonon polaron branch, (solid) and (dashed) vs for , .

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/content/aip/journal/pop/12/7/10.1063/1.1937421
2005-06-29
2014-04-23
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: THz instability by streaming carriers in high mobility solid-state plasmas
http://aip.metastore.ingenta.com/content/aip/journal/pop/12/7/10.1063/1.1937421
10.1063/1.1937421
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