On February 16, 1983, during a period of strong magnetic disturbance (Kp~5), as the ISEE 1 satellite passed near the magnetic meridian of the Omega navigation transmitter (98¿W, 46¿N geographic, L~3.4), the Stanford University VLF wave receiver detected the presence of Omega transmitter signals over the range 2≤L≤3.7 at magnetic latitudes (&lgr;m) within 10¿ of the magnetic equator. Over a 500-km orbital segment near L~3.4 and &lgr;m~5¿S, the electric field amplitude of the Omega signals reached ~0.6 mV/m, a value >40dB higher than the signal amplitude both preceding (L~3.7--3.5) and following (L≤3.2) the high-amplitude period.

Over the range 3.3≤L≤3.7 the transmitter pulses at 13.1 and 13.6 kHz were associated with sideband signals spaced in frequency roughly symmetrically about the carrier and generally reduced in amplitude ~5 dB with respect to the carrier. The strongest sidebands were generally offset in frequency from the carrier by ~¿55 Hz. Simultaneous data from the University of Iowa Plasma Wave experiment indicated that the region of high wave amplitude was located just beyond the outer edge of the plasmapause where low values of cold plasma density (~40 el/cm3) prevailed. High amplitudes were observed only during the time in which the signal frequency lay within the range of a natural noise band of rising center frequency in which bursts of VLF emissions were occasionally triggered by ''knee-trace'' whistlers. On the basis of the group time delay and amplitude distribution of the Omega signals and the presence off knee-trace whistlers, it is concluded that the high amplitude signals originally propagated along the base of the plasmapause surface into the southern hemisphere and subsequently reflected or scattered back up to the satellite. The high-wave amplitude was presumably produced through the coherent whistler mode instability as the input waves interacted with gyroresonant energetic electrons near the magnetic equatorial plane, and the presence of sideband signals indicates that this interaction had reached a nonlinear stage.

The wave magnetic field in the interaction region is estimated to be approximately 20 m&ggr;. The high amplitudes reached by the signals indicates that particle trapping effects could be responsible for the sideband generation.