Magnetospheric amplification and emission triggering by ELF/VLF waves injected by the 3.6 MW HAARP ionospheric heater

[1] The HF dipole array of the High Frequency Active Auroral Research Program (HAARP) in Gakona, Alaska, was recently upgraded to 180 elements, facilitating operations at a total radiated power level of 3.6 MW and an effective radiated power of ∼575 MW. In the first experiments at the new power level, the HAARP array is used for magnetospheric wave injection. Modulated heating of auroral electrojet currents in the ionosphere yields radiation in the ELF/VLF frequency range. The HAARP-generated signals are injected into the magnetosphere, where they propagate in the whistler mode in field-aligned "ducts," allowing them to be observed at the conjugate point on a ship-borne receiver and on autonomous buoy platforms. The observation of the 1-hop signals is accompanied by the observation of associated 2-hop components in the northern hemisphere, which have reflected from the ionospheric boundary in the southern hemisphere. The observed signals are accompanied by triggered emissions and exhibit temporal amplification of 15-25 dB/s and bandwidth broadening to ∼50 Hz. Amplification occurs at injected signal frequencies selected in near real time on the basis of observations of natural emission activity, and only certain components of the frequency-time formats transmitted are amplified. Observations at multiple sites and dispersion analysis show that the signals are injected into the magnetosphere directly above the HF heater. The duration of echo observation and the prevalence of 1-hop observations are consistent with statistics from 1986 Siple Station experiments. The particle-trapping wave amplitude near the magnetic equator is estimated in the range 0.1-0.4 pT and gyroresonance with 10 keV-100 keV electrons.

[1]  G. S. Stiles,et al.  Frequency‐time behavior of artificially stimulated VLF emissions , 1975 .

[2]  D. Nunn A SELF-CONSISTENT THEORY OF TRIGGERED VLF EMISSIONS , 1974 .

[3]  R. Anderson,et al.  An ISEE/Whistler model of equatorial electron density in the magnetosphere , 1992 .

[4]  E. Nielsen,et al.  The characteristics of ionospheric heating-produced ELF/VLF waves over 32 hours , 1987 .

[5]  Umran S. Inan,et al.  DEMETER observations of ELF waves injected with the HAARP HF transmitter , 2006 .

[6]  D. L. Carpenter,et al.  Rare ground‐based observations of Siple VLF transmitter signals outside the plasmapause , 1983 .

[7]  Umran S. Inan,et al.  Orientation of the HAARP ELF ionospheric dipole and the auroral electrojet , 2008 .

[8]  D. L. Carpenter,et al.  Ducted magnetospheric propagation of signals from the Siple, Antarctica, VLF transmitter , 1976 .

[9]  R. Helliwell,et al.  VLF wave stimulation experiments in the magnetosphere from Siple Station, Antarctica , 1988 .

[10]  Umran S. Inan,et al.  Multistation observations of ELF/VLF whistler mode chorus , 2008 .

[11]  R. Helliwell,et al.  Variable frequency VLF signals in the magnetosphere: Associated phenomena and plasma diagnostics , 1985 .

[12]  R. Helliwell,et al.  Power threshold for growth of coherent VLF signals in the magnetosphere , 1980 .

[13]  G. G. Getmantsev,et al.  Combination frequencies in the interaction between high-power short-wave radiation and ionospheric plasma , 1974 .

[14]  M. Rietveld,et al.  On the frequency dependence of ELF/VLF waves produced by modulated ionospheric heating , 1989 .

[15]  U. Inan,et al.  Radiation of ELF/VLF waves by harmonically varying currents into a stratified ionosphere with application to radiation by a modulated electrojet , 2008 .

[16]  M. Rycroft,et al.  Multi-station VLF direction-finding measurements in eastern Canada , 1982 .

[17]  J. J. Angerami,et al.  Whistler studies of the plasmapause in the magnetosphere: 2. Electron density and total tube electron content near the knee in magnetospheric ionization , 1966 .

[18]  Michael T. Rietveld,et al.  ELF and VLF wave generation by modulated HF heating of the current carrying lower ionosphere , 1982 .

[19]  R. Barr,et al.  ELF radiation from the Tromsø “Super Heater” Facility , 1991 .

[20]  Peter Stubbe,et al.  ELF and VLF radiation from the polar electrojet antenna , 1984 .

[21]  R. Helliwell,et al.  VLF wave injection into the magnetosphere from Siple Station, Antarctica , 1974 .

[22]  D. L. Carpenter,et al.  Ducted whistler propagation outside the plasmapause , 1988 .

[23]  M. K. Andrews,et al.  Magnetospheric electric fields and protonospheric coupling fluxes inferred from simultaneous phase and group path measurements on whistler-mode signals , 1978 .

[24]  Sergei Sazhin,et al.  Whistler diagnostics of magnetospheric parameters: A review , 1992 .

[25]  R. Helliwell A theory of discrete VLF emissions from the magnetosphere , 1967 .

[26]  Umran S. Inan,et al.  DEMETER observations of an intense upgoing column of ELF/VLF radiation excited by the HAARP HF heater , 2008 .

[27]  Umran S. Inan,et al.  ELF waves generated by modulated HF heating of the auroral electrojet and observed at a ground distance of ∼4400 km , 2007 .

[28]  Koichiro Tsuruda,et al.  High spatial attenuation of the Siple transmitter signal and natural VLF chorus observed at ground‐based chain stations near Roberval, Quebec , 1982 .

[29]  Umran S. Inan,et al.  Multi‐hop whistler‐mode ELF/VLF signals and triggered emissions excited by the HAARP HF heater , 2004 .

[30]  H. Matsumoto,et al.  A review of observational, theoretical and numerical studies of VLF triggered emissions , 1991 .

[31]  T. Bell,et al.  Simultaneous triggered VLF emissions and energetic electron distributions observed on POLAR with PWI and HYDRA , 2000 .