Abstract

Abstract. Data from the Jicamarca digisonde and the ROCSAT-1 satellite are employed to study the equatorial ionosphere on the west side of South America during April 1999-March 2000 for the concurrent bottomside spread F (BSSF) and plasma bubble events. This study, using digisonde and ROCSAT-1 concurrently, is the first attempt to investigate the equatorial spread F. Results show that BSSF and plasma bubble observations appear frequently respectively in the summer (January, February, November, and December) and in the equinoctial (March, April, September, and October) months, respectively, but are both rarely observed in the winter (May-August) months. The upward drift velocity during the concurrent BSSF and bubble observations has been determined to study the driving mechanism. This analysis shows that large vertical drift velocities favor BSSF and bubble formations in the equinoctial and summer months. Conversely, the smaller upward velocities during the winter months cause fewer BSSF and bubble occurrences. For the geomagnetic effect, the BSSF/bubble occurrence decreases with an increasing Kp value in the equinoctial months, but no such correlation is found for the summer and winter months. Moreover, the anti-correlations between Kp and dh'F/dt are apparent in the equinoctial months, but not in the summer and winter months. These results indicate that in the equinoctial months the BSSF/bubble generations and the pre-reversal drift velocity can be suppressed by geomagnetic activity, because the disturbance dynamo effects could have decreased the eastward electric field near sunset. However, BSSF and bubble occurrences may not be suppressed by the geomagnetic activity in the summer and winter months.

Highlights

  • Plasma irregularities and inhomogeneities in the equatorial F region caused by plasma instabilities are called the equatorial spread F (ESF) (e.g. Kelley, 1989)

  • The bottomside spread F (BSSF) occurrence is higher in the summer (November, December, January, and February)/the equinoctial months, than in the winter months (May, June, July, and August)

  • The occurrence dependences of BSSF and bubble formation on season, dh F /dt, and Kp were examined in the work

Read more

Summary

Introduction

Plasma irregularities and inhomogeneities in the equatorial F region caused by plasma instabilities are called the equatorial spread F (ESF) (e.g. Kelley, 1989). Little work has been published examining the simultaneous occurrence of BSSF and bubble in the equatorial ionosphere (Whalen, 1997, 2002) In his first report, Whalen (1997) compared the monthly occurrence of bubble with that of BSSF during solar maximum, using a chain of ionospheric sounders in the western American sector. Whalen (2002) employed the same data set to study the dependence of BSSF and bubble occurrences on season, the geomagnetic activity, and the E×B drift velocity. Whalen (1997, 2002) simultaneously investigated the BSSF and bubble formations in the equatorial ionosphere, he did not use satellite data or estimated the vertical drift velocity from his data set. We have used these data to examine the dependence of the BSSF and bubble occurrences on season, the E×B drift velocity, and the geomagnetic activity (Kp) in the current study

Experiment setup
Seasonal occurrences of BSSF and bubble formation
Geomagnetic effect on the occurrence of BSSF and bubble formation
Summary and conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call