PROPERTIES OF THE MAGNETOSPHERIC HOT PLASMA DISTRIBUTION DEDUCED FROMWHISTLER-MODE WAVE INJECTION AT 2400 HZ - GROUND-BASED DETECTION OF AZIMUTHAL STRUCTURE IN MAGNETOSPHERIC HOT PLASMAS
Vs. Sonwalkar et al., PROPERTIES OF THE MAGNETOSPHERIC HOT PLASMA DISTRIBUTION DEDUCED FROMWHISTLER-MODE WAVE INJECTION AT 2400 HZ - GROUND-BASED DETECTION OF AZIMUTHAL STRUCTURE IN MAGNETOSPHERIC HOT PLASMAS, J GEO R-S P, 102(A7), 1997, pp. 14363-14380
Siple station VLF wave injection experiments aimed at finding the prop
erties of the magnetospheric hot plasma were conducted for a 9-hour pe
riod between 1705 and 0210 UT on January 23-24, 1988. A special freque
ncy versus time format, lasting 1 min and transmitted every 5 min, con
sisted of a sequence of pulses, frequency ramps, and parabolas, all in
a 1-kHz range centered on 2400 Hx. The transmitted signals, after pro
pagating along a geomagnetic field-aligned duct, were recorded at Lake
Mistissini, Canada. At various times during the 9-hour interval the S
iple signals showed features characteristic of wave-particle interacti
ons, including wave growth, sidebands, and triggered emissions. Our ob
servations, primarily at 2400 Hz, show that (1) there were no correlat
ions between the initial levels, the growth rates, and the saturation
levels of constant-frequency pulses; (2) in general, the values of gro
wth rate and saturation level of two pulses injected within 30 s were
nearly the same; (3) the initial level, growth rate, and saturation le
vel showed temporal variations over 5-15 min and 1-2 hour timescales;
(4) the leading edges of constant-frequency signals underwent spatial
amplification; and (5) under conditions of saturation the received sig
nal bandwidth (similar to 20 Hz) remained constant over a 1-hour perio
d, although the saturation level and growth rate varied during the sam
e period. On the assumption that gyroresonant interactions were respon
sible for the observed wave growth and saturation, the timescales over
which those phenomena varied provide constraints on the possible ener
getic electron population within the duct. In the reference frame of t
he duct (L similar to 5.1, N-e similar to 280 cm(-3)) the particle flu
xes showed no variation over a 30-s timescale but varied over 5-15 min
and 1-2 hour timescales. The 5-15 min timescale variations indicate l
ongitudinal structures ranging from similar to 0.20 or similar to 100
km (in the equatorial plane) for electrons with energy E = 0.6 keV and
pitch angle alpha = 40 degrees, to similar to 5 degrees or similar to
2800 km for electrons with energy E = 11 keV and pitch angle alpha =
80 degrees. The hour-long time variations indicate longitudinal struct
ures ranging from similar to 2 degrees or similar to 1100 km (in the e
quatorial plane) for electrons with energy E = 0.6 keV and pitch angle
alpha = 40 degrees, to similar to 45 degrees or similar to 25,000 km
for electrons with energy E = 11 keV and pitch angle alpha = 80 degree
s. We conclude that ground-based active and passive wave experiments h
ave substantial potential for investigating properties of the hot plas
ma of the magnetosphere.