Abstract

Abstract. A comparison of HF radar backscatter observed by the CUTLASS Finland radar, meridian scanning photometer data from Longyearbyen, magnetic field variations from IMAGE stations, and particle precipitation measured by the DMSP F12 spacecraft is presented. The interval under discussion occurred in the pre-midnight local time sector, during a period of weakly northward interplanetary magnetic field. A region of HF backscatter, typically 8 degrees wide, occurred in the field of view of the CUTLASS Finland radar. A well defined gradient in the spectral width parameter was present, with mainly low (< 200 m s - 1 ) spectral widths in the lower latitude part of the scatter and predominantly large (> 200 ms - 1 ) spectral widths in the higher latitude part. The relationship between the spectral width and the red line (630.0 nm) emission measured by the meridian scanning photometer is considered. The poleward border of the red line emission, which has, in the past, been proposed as being representative of the polar cap boundary, was co-located to within 1° of magnetic latitude with the gradient in spectral width for part of the interval. Statistically, large spectral widths occurred poleward of the red line emission, while small spectral widths occurred within or equatorward of the red line emission. Near simultaneous DMSP particle observations in the 20 eV to 20 keV range indicate that the poleward border of the red line emission and the gradient in spectral width occurred at the same latitude as the transition from auroral oval to polar rain particle energies. We conclude that the large spectral widths were not caused by particle precipitation associated with the auroral oval. There were two periods of special interest when the relationship between the red line and the spectral width broke down. The first of these happened during enhanced red line and green line (557.7 nm) emission, with a drop out of the radar scatter and an enhanced, narrow westward electrojet. We conclude that this event was a magnetospheric substorm occurring at much higher than usual latitudes. The second period of special interest happened when equatorward moving bands of large spectral width occurred within the region of scatter. Up to 4 of these bands were present during an interval of 100 minutes. Associated with these narrow bands of large spectral width were narrow channels of enhanced westward ion velocities. We conclude that these equatorward moving bands of large spectral width may be related to reconnection processes in the tail. The observations demonstrate that the tail continues to be active even under low solar wind energy input conditions. Furthermore, we conclude that the gradient in the spectral width may be used as a proxy for the polar cap boundary, but only with extreme caution.Key words. Ionosphere (ionosphere-magnetosphere inter-actions; polar ionosphere) – Magnetospheric physics (storms and substorms)

Highlights

  • The boundary between open and closed magnetic field lines, when mapped into the ionosphere, is often termed the polar cap boundary. The motion of this boundary, and the size of the polar cap and the amount of open flux in the magnetosphere, in response to solar wind, interplanetary magnetic field (IMF) conditions, and magnetospheric substorms is a topic of considerable interest

  • The effect of the viscous interaction during southward IMF Bz is to move the centre of the two flow cells to lower latitudes, thereby displacing the flow reversal boundary (FRB) from the boundary between open and closed magnetic flux, i.e. the polar cap boundary (PCB)

  • We find that in this particular case study there is evidence that a gradient in spectral width is related to the PCB, with large spectral widths co-located with polar rain electron precipitation poleward of the PCB

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Summary

Introduction

The boundary between open and closed magnetic field lines, when mapped into the ionosphere, is often termed the polar cap boundary. The effect of the viscous interaction during southward IMF Bz is to move the centre of the two flow cells to lower latitudes, thereby displacing the flow reversal boundary (FRB) from the boundary between open and closed magnetic flux, i.e. the polar cap boundary (PCB). To gain a quantitative understanding of how the open magnetic flux in the magnetosphere varies as a function of the IMF and substorm activity, it is necessary to be able to follow the location of the PCB at all local times. The particle distributions measured by low earth orbiting spacecraft, such as DMSP and FAST, can be used to identify the boundary between auroral precipitation and polar rain This represents one diagnostic for the PCB

Experimental overview
Observations
40 HOP 20
Discussion
High-latitude substorm onset
High spectral width boundary
Polar cap boundary definition
Polar cap boundary and spectral width
Polar cap boundary and flow reversal boundary
High spectral width and particle precipitation
Findings
Equatorward moving bands
Conclusions
Full Text
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