Physics
Scientific paper
Jan 2011
adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=2011jastp..73..164t&link_type=abstract
Journal of Atmospheric and Solar-Terrestrial Physics, Volume 73, Issue 1, p. 164-177.
Physics
2
Scientific paper
Two high speed stream (HSS) solar wind intervals (days 283-294 and 314-318, 2003, hereafter called Events 1 and 2) during the declining phase of solar cycle 23 have been examined in detail for their interplanetary characteristics and their resultant geomagnetic activity. Event 1 had an associated storm initial phase with peak Dst=+9 nT. This was caused by a high plasma density heliospheric plasma sheet (HPS) which impacted the magnetosphere. The southward component of IMF Bz fluctuations in the corotating interaction regions (CIRs) of both Events 1 and 2 led to peak storm main phases of Dst=-85 and -62 nT, respectively. The extended storm “recovery” phases were associated with ΔB/Bo ˜1-2 Alfvénic fluctuations in the HSS proper. High-intensity, long-duration, continuous AE (HILDCAA) intervals were present, presumably due to the southward component of the Alfvén waves. The IMF Bx-Vx 4-h cross-correlation values were >0.8 in Event 2, and lower, >0.6, in Event 1. The difference in Alfvénicity between the two HSS events is not understood at present. The IMF Bz 10-min to 3-h variances (σz2) and are highest during the CIRs. The normalized variances (σz2/Bo2) during the HSS proper are approximately the same as those for the CIRs. For Event 1, the 1-h IMF σz2 and σz2/Bo2 are 5.0 nT2 and 1.1×10-1, respectively. The IMF Bz-AE cross-correlation (c.c.) coefficients during the storm main phase of Event 1 and for 24-h of the HSS of Event 2 give similar results. For the Event 1, a peak c.c. of -0.4 occurred with a lag of 103 min, and for Event 2 a peak c.c of -0.38 with a lag of 67 min was obtained. Both c.c. results were sharply peaked. The decay-portion of a HSS prior to Event 1 was characterized by low Np, low Bo and low Alfvén wave amplitudes. The 1-h IMF σz2 and σz2/Bo2 were 0.84 nT2 and 2.9×10-2, respectively. This quiet interplanetary interval led to a quiet geomagnetic activity period (AE<100 nT, Dst ˜+5 nT). On the other hand, what is quite surprising is that this region was the most purely “Alfvénic” interval studied (c.c. of Bx-Vx=0.95). The ɛ parameter was calculated using both GSE and GSM coordinates. It was found that ɛ is ˜30% larger for GSM coordinates. Thus, the major cause of geomagnetic activity during HSSs is the large amplitude Alfvén waves but not coordinate transformations. Sector polarities (IMF By values) may be a secondary factor. However, other models, like the tilted solar dipole, should be considered as well.
Echer Ezequiel
Gonzalez Walter D.
Guarnieri Fernando Luís
Tsurutani Bruce T.
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