@InProceedings{karney81a,
author = {Charles F. F. Karney},
title = {Temporal Evolution of Nonlinear Lower Hybrid Waves},
booktitle = {Heating in Toroidal Plasmas},
pages = {455-461},
year = 1981,
editor = {E. Canobbio and H. P. Eubank and G. G. Leotta and
A. Malein and E. Sindoni},
volume = {I},
publisher = {Commission of the European Communities, Brussels,
Belgium (EUR 7424 EN)},
reprint = {htp81},
note = {Proc. Second Joint Varenna--Grenoble International
Symposium, Como, Italy, Sept. 3--12, 1980},
abstract = {The nonlinear evolution of a single lower hybrid wave
in two dimensions and time is considered. If the
potential is taken to have the form φ(<i>x</i>,
<i>z</i>, <i>t</i> )
exp(−<i>i</i>ω<i>t</i> ), the
equation describing the fields is
<i>i</i><i>v</i><sub>τ</sub> − ∫
<i>v</i><sub>ξ</sub> <i>d</i>ζ +
<i>v</i><sub>ζζ</sub> +
|<i>v</i>|<sup>2</sup><i>v</i> = 0 where <i>v</i> is
proportional to the electric field, τ to time, and
ξ and ζ measure distances across and along the
lower hybrid ray. The properties of this equation are
investigated numerically. When the amplitude of the
injected lower hybrid waves is sufficiently large, the
following phenomena are observed: the fields do not
reach a steady state even though steady-state boundary
conditions are imposed; the density modulations are
sufficient to cause an appreciable fraction of the
incident power to be reflected; the average wavenumber
of the transmitted wave is larger than that of the
incident wave.}
}