Abstract

Abstract. A previous case study found a relationship between high spectral width measured by the CUTLASS Finland HF radar and elevated electron temperatures observed by the EISCAT and ESR incoherent scatter radars in the post-midnight sector of magnetic local time. This paper expands that work by briefly re-examining that interval and looking in depth at two further case studies. In all three cases a region of high HF spectral width (>200 ms-1) exists poleward of a region of low HF spectral width (<200 ms-1). Each case, however, occurs under quite different geomagnetic conditions. The original case study occurred during an interval with no observed electrojet activity, the second study during a transition from quiet to active conditions with a clear band of ion frictional heating indicating the location of the flow reversal boundary, and the third during an isolated sub-storm. These case studies indicate that the relationship between elevated electron temperature and high HF radar spectral width appears on closed field lines after 03:00 magnetic local time (MLT) on the nightside. It is not clear whether the same relationship would hold on open field lines, since our analysis of this relationship is restricted in latitude. We find two important properties of high spectral width data on the nightside. Firstly the high spectral width values occur on both open and closed field lines, and secondly that the power spectra which exhibit high widths are both single-peak and multiple-peak. In general the regions of high spectral width (>200 ms-1) have more multiple-peak spectra than the regions of low spectral widths whilst still maintaining a majority of single-peak spectra. We also find that the region of ion frictional heating is collocated with many multiple-peak HF spectra. Several mechanisms for the generation of high spectral width have been proposed which would produce multiple-peak spectra, these are discussed in relation to the data presented here. Since the regions of high spectral width are observed both on closed and open field lines the use of the boundary between low and high spectral width as an ionospheric proxy for the open/closed field line boundary is not a simple matter, if indeed it is possible at all.Key words. Ionosphere (auroral ionosphere; ionospheric irregularities)

Highlights

  • The Doppler spectral width parameter observed by coherent HF radars is associated with the turbulent characteristics of the plasma irregularities being illuminated by the radar

  • The spectral width parameter observed by the Super Dual Auroral Radar Network (SuperDARN) coherent HF radars (Greenwald et al, 1995), has been used as an ionospheric proxy for the position of the low-altitude cusp on the dayside

  • This paper extends the work by Woodfield et al (2002), briefly revisiting the first case study, and introducing two further case studies and looking in more detail at the power spectra from the received backscatter

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Summary

Introduction

The Doppler spectral width parameter observed by coherent HF radars is associated with the turbulent characteristics of the plasma irregularities being illuminated by the radar. It is thought that within the cusp region the spectral width is high (> 150 ms−1) and variable (Baker et al, 1990, 1995; Pinnock et al, 1995, Andreet al., 1999, 2000a; Milan et al, 1999; Moen et al, 2001; Rodger, 2000; Milan and Lester, 2001; Pinnock and Rodger, 2001), this is not always the case (Rodger et al, 1995) This feature is believed to be the result of the problems that the standard parameter fitting software (FITACF) (Villain et al, 1987) has fitting auto-correlation functions (ACFs) which lead to power spectra that have several large peaks. The spectral width and line-of-sight velocity are both more variable where the spectra have multiple-peaks, and the errors associated with the fitting of these parameters are increased

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