The electron energy distribution during HF pumping, a picture painted with all colors.

Abstract. The shape of the electron energy distribution has long been a central question in the field of high-frequency radio-induced optical emission experiments. This report presents estimates of the electron energy distribution function, fe(E), from 0 to 60 eV, based on optical multi-wavelength (6300, 5577, 8446, 4278A) data and 930-MHz incoherent scatter radar measurements of ion temperature, electron temperature and electron concentration. According to our estimate, the electron energy distribution has a depression at around 2 eV, probably caused by electron excitation of vibrational states in N2, and a high energy tail that is clearly supra-thermal. The temporal evolution of the emissions indicates that the electron temperature still plays an important role in providing electrons with energies close to 2 eV. At the higher energies the electron energy distribution has a non-thermal tail. Keywords. Active experiments; Ionosphere atmosphere interaction; Ionospheric physics

[1]  P. Bernhardt,et al.  Artificial Airglow Excited by High-Power Radio Waves , 1988, Science.

[2]  M. Rietveld,et al.  Introduction to ionospheric heating at Tromsø—I. Experimental overview , 1993 .

[3]  A. Hedin Extension of the MSIS Thermosphere Model into the middle and lower atmosphere , 1991 .

[4]  G. Milikh,et al.  Multiple acceleration of electrons in the regions of high-power radio-wave reflection in the ionosphere , 1985 .

[5]  Craig A. Tepley,et al.  Airglow enhancements associated with plasma cavities formed during Ionospheric Heating Experiments , 1989 .

[6]  H. Carlson,et al.  Suprathermal electrons generated by the interaction of powerful radio wave with the ionosphere , 2000 .

[7]  R. Laher,et al.  Franck-Condon factors, r-centroids electronic transition moments, and Einstein coefficients for many nitrogen and oxygen band systems. Technical report, 1 Dec 89-30 Sep 91 , 1992 .

[8]  Measurements of the 237 Np(n,f) Cross Section , 1994 .

[9]  W. J. Burke,et al.  On the Onset of HF-Induced Airglow at HAARP , 2004 .

[10]  D. Russell,et al.  Caviton dynamics in strong Langmuir turbulence , 1990 .

[11]  Y. Itikawa,et al.  Cross Sections for Collisions of Electrons and Photons with Atomic Oxygen , 1990 .

[12]  T. Yeoman,et al.  Ionospheric electron heating, optical emissions, and striations induced by powerful HF radio waves at high latitudes: Aspect angle dependence , 2003 .

[13]  J. P. Doering,et al.  Absolute differential and integral electron excitation cross sections for atomic oxygen 7. The 3 P → 1 D and 3 P → 1 S transitions from 4.0 to 30 eV , 1989 .

[14]  F. Honary,et al.  Analysis of excitation of the 630.0 nm airglow during a heating experiment in Tromsø on February 16, 1999 , 2000 .

[15]  G. Milikh,et al.  Artificial airglow due to modifications of the ionosphere by powerful radio waves , 1997 .

[16]  H. Carlson,et al.  Observations of fluxes of suprathermal electrons accelerated by HF excited instabilities , 1982 .

[17]  G. P. Mantas Large 6300‐Å airglow intensity enhancements observed in Ionosphere Heating Experiments are excited by thermal electrons , 1994 .

[18]  J. Weinstock Theory of enhanced airglow during ionospheric modifications , 1975 .

[19]  Michael Kosch,et al.  High‐latitude HF‐induced airglow displaced equatorwards of the pump beam , 2000 .

[20]  F. Honary,et al.  Simulation of high energy tail of electron distribution function , 2004 .

[21]  A. Aruliah,et al.  First tomographic estimate of volume distribution of HF-pump enhanced airglow emission , 2001 .

[22]  F. Honary,et al.  Simultaneous measurements of high-frequency pump-enhanced airglow and ionospheric temperatures at auroral latitudes , 2000 .

[23]  L. S. Wagner,et al.  Optical remote sensing of the thermosphere with HF pumped artificial airglow , 2000 .

[24]  J. P. Doering,et al.  Absolute differential and integral electron excitation cross sections for atomic nitrogen , 1991 .

[25]  T. Hagfors,et al.  High‐latitude pump‐induced optical emissions for frequencies close to the third electron gyro‐harmonic , 2002 .

[26]  R. Johnsen,et al.  Measurements of the O+ + N2 and O+ + O2 reaction rates from 300°K to 2 eV , 1973 .

[27]  M. Goldman,et al.  Vlasov simulations of electron heating by Langmuir turbulence near the critical altitude in the radiation-modified ionosphere , 1997 .

[28]  Russ R. Laher,et al.  Franck–Condon Factors, r‐Centroids, Electronic Transition Moments, and Einstein Coefficients for Many Nitrogen and Oxygen Band Systems , 1992 .

[29]  P. Kaw,et al.  On the role of plasma instabilities in ionospheric heating by radio waves , 1971 .

[30]  R. Johnsen,et al.  Measurements of the O++N2 and O++O2 reaction rates from 300 to 900 K , 1978 .

[31]  Hiroaki Nishimura,et al.  Cross Sections for Collisions of Electrons and Photons with Oxygen Molecules , 1986 .

[32]  T. Leyser,et al.  Unambiguous evidence of HF pump‐enhanced airglow at auroral latitudes , 1999 .

[33]  T. Hagfors,et al.  A new digital all-sky imager experiment for optical auroral studies in conjunction with the Scandinavian twin auroral radar experiment , 1998 .

[34]  P. Bernhardt,et al.  Heater-induced cavities as optical tracers of plasma drifts , 1989 .

[35]  H. Carlson,et al.  First observations of HF heater‐produced airglow at the High Frequency Active Auroral Research Program facility: Thermal excitation and spatial structuring , 2001 .

[36]  T. Aso,et al.  ALIS- A Multi-Station Imaging System at High Latitudes with Multi-Disciplinary Scientific Objectives , 1997 .

[37]  T. Leyser,et al.  Nearly simultaneous images of HF‐pump enhanced airglow at 6300 Å and 5577 Å , 2002 .

[38]  L. Megill,et al.  A model of the enhanced airglow excited by RF radiation , 1974 .

[39]  U. Brändström The Auroral Large Imaging System : design, operation and scientific results , 2003 .

[40]  J. Weinstock,et al.  Theory of Electron Acceleration during Parametric Instabilities , 1974 .

[41]  J. P. Doering Absolute differential and integral electron excitation cross sections for atomic oxygen: 9. Improved cross section for the ³P → ¹D transition from 4.0 to 30 eV , 1992 .

[42]  M. Hayashi,et al.  Cross Sections for Collisions of Electrons and Photons with Nitrogen Molecules , 1985 .

[43]  H. Carlson,et al.  Reinterpretation of the 6300‐Å airglow enhancements observed in ionosphere heating experiments based on analysis of Platteville, Colorado, data , 1996 .

[44]  R. Hake,et al.  Optical (λ6300) detection of radio frequency heating of electrons in the F region , 1970 .

[45]  Herbert C. Carlson,et al.  On the electron distribution function in the F region and airglow enhancements during HF modification experiments , 2000 .