Investigation of subauroral ion drifts and related field-aligned currents and ionospheric Pedersen conductivity distribution

Abstract. Based on Astrid-2 satellite data, results are presented from a statistical study on subauroral ion drift (SAID) occurrence. SAID is a subauroral phenomenon characterized by a westward ionospheric ion drift with velocity greater than 1000m/s, or equivalently, by a poleward-directed electric field with intensity greater than 30mV/m. SAID events occur predominantly in the premidnight sector, with a maximum probability located within the 20:00 to 23:00 MLT sector, where the most rapid SAID events are also found. They are substorm related, and show first an increase in intensity and a decrease in latitudinal width during the expansion phase, followed by a weakening and widening of the SAID structures during the recovery phase. The potential drop across a SAID structure is seen to remain roughly constant during the recovery phase. The field-aligned current density and the height-integrated Pedersen conductivity distribution associated with the SAID events were calculated. The results reveal that the strongest SAID electric field peaks are associated with the lowest Pedersen conductivity minimum values. Clear modifications are seen in the ionospheric Pedersen conductivity distribution associated with the SAID structure as time evolves: the SAID peak is located on the poleward side of the corresponding region of reduced Pedersen conductivity; the shape of the regions of reduced conductivity is asymmetric, with a steeper poleward edge and a more rounded equatorward edge; the SAID structure becomes less intense and widens with evolution of the substorm recovery phase. From the analysis of the SAID occurrence relative to the mid-latitude trough position, SAID peaks are seen to occur relatively close to the corresponding mid-latitude trough minimum. Both these features show a similar response to magnetospheric disturbances, but on different time scales - with increasing magnetic activity, the SAID structure shows a faster movement towards lower latitudes than that of the mid-latitude trough. From the combined analysis of these results, we conclude that the SAID generation mechanism cannot be regarded either as a pure voltage generator or as a pure current generator, applied to the ionosphere. While the anti-correlation between the width and the peak intensity of the SAID structures with substorm evolution indicates a magnetospheric source acting as a constant voltage generator, the ionospheric modifications and, in particular the reduction in the conductivity for intense SAID structures, are indicative of a constant current system closing through the ionosphere. The ionospheric feedback mechanisms are seen to be of major importance for sustaining and regulating the SAID structures. Key words. Ionosphere (mid-latitude ionosphere; electric fields and currents; ionosphere-magnetosphere interactions)

[1]  Y. Galperin Polarization Jet: characteristics and a model , 2002 .

[2]  P. Anderson,et al.  Multisatellite observations of rapid subauroral ion drifts (SAID) , 2001 .

[3]  Y. Galperin,et al.  Formation of a Polarization Jet during the Expansion Phase of a Substorm: Results of Ground-Based Measurements , 2001 .

[4]  W. J. Burke,et al.  Ionospheric disturbances observed by DMSP at middle to low latitudes during the magnetic storm of June 4–6, 1991 , 2000 .

[5]  J. Keyser Formation and evolution of subauroral ion drifts in the course of a substorm , 1999 .

[6]  L. Blomberg,et al.  Astrid-2: An Advanced Auroral Microprobe , 1999 .

[7]  J. Lemaire,et al.  The magnetospheric driver of subauroral ion drifts , 1998 .

[8]  L. Blomberg,et al.  Subauroral electric fields observed by the Freja satellite: A statistical study , 1998 .

[9]  J. Foster,et al.  Predicting plasmaspheric radial density profiles , 1997 .

[10]  G. W. Prölss,et al.  The position of the ionospheric trough as a function of local time and magnetic activity , 1997 .

[11]  Hermann Lühr,et al.  An algorithm for estimating field-aligned currents from single spacecraft magnetic field measurements: a diagnostic tool applied to Freja satellite data , 1996, IEEE Trans. Geosci. Remote. Sens..

[12]  P. Anderson,et al.  A proposed production model of rapid subauroral ion drifts and their relationship to substorm evolution , 1993 .

[13]  R. Hoffman,et al.  Finite geometry effects of field-aligned currents , 1992 .

[14]  S. Quegan,et al.  The role of ion drift in the formation of ionisation troughs in the mid- and high-latitude ionosphere—a review , 1992 .

[15]  P. Anderson,et al.  The ionospheric signatures of rapid subauroral ion drifts , 1991 .

[16]  W. J. Burke,et al.  Quantitative simulation of a magnetospheric substorm 2. Comparison with observations , 1981 .

[17]  R. W. Spiro,et al.  Quantitative simulation of a magnetospheric substorm 1. Model logic and overview , 1981 .

[18]  N. Maynard,et al.  Magnetospheric observation of large sub-auroral electric fields , 1980 .

[19]  W. J. Burke,et al.  Observations of field‐aligned currents in association with strong convection electric fields at subauroral latitudes , 1980 .

[20]  R. Heelis,et al.  Rapid subauroral ion drifts observed by Atmosphere Explorer C , 1979 .

[21]  P. Banks,et al.  Electric fields and conductivity in the nighttime E-region: A new magnetosphere-ionosphere-atmosphere coupling effect , 1978 .

[22]  R. Wolf,et al.  An assessment of the role of precipitation in magnetospheric convection , 1978 .

[23]  N. Maynard On large poleward-directed electric fields at sub-auroral latitudes , 1978 .

[24]  J. Hoffman,et al.  Ionospheric and magnetospheric plasmapauses , 1978 .

[25]  J. Whitteker,et al.  Plasmapause signatures in the ionosphere and magnetosphere , 1978 .

[26]  W. J. Burke,et al.  Intense poleward‐directed electric fields near the ionospheric projection of the plasmapause , 1977 .

[27]  R. Schunk,et al.  Effects of electric fields and other processes upon the nighttime high-latitude F layer , 1976 .