1992
DOI: 10.1029/92gl01312
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Low‐energy solar electrons and ions observed at Ulysses February‐April, 1991: The inner heliosphere as a particle reservoir

Abstract: Ulysses observations at 2.5 AU of 38–315 keV electrons and 61–4752 keV ions during February‐April 1991 suggest in several ways that, during periods of sustained high solar activity, the inner heliosphere serves as a “reservoir” for low‐energy solar particles. Particle increases were not associated one‐to‐one with large X‐ray flares because of their poor magnetic connection, yet intensities in March‐April remained well above their February levels. The rise phase of the particle event associated with the great f… Show more

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Cited by 113 publications
(84 citation statements)
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“…The transit time for a 63 keV electron with zero-degree pitch-angle along an ideal spiral to 2.5 AU (i.e., a curvilinear distance of 3.3 AU for a solar wind velocity of 650 km/s) is one hour. Roelof et al (1992) state that the reason the rise is nearly velocity dispersionless with a near-constant spectrum is that the transit times for these particles are considerably shorter than the rise time of 3.1 h. Thus, the electrons easily populate the¯ux tube to 2.5 AU faster than their rate of injection. On March 23, Ulysses was located at a distance of 2.5 AU from the Sun, and the Ulysses footpoint mapped back to a longitude of ~W60°on the Sun as viewed from the Earth.…”
Section: Discussionmentioning
confidence: 99%
“…The transit time for a 63 keV electron with zero-degree pitch-angle along an ideal spiral to 2.5 AU (i.e., a curvilinear distance of 3.3 AU for a solar wind velocity of 650 km/s) is one hour. Roelof et al (1992) state that the reason the rise is nearly velocity dispersionless with a near-constant spectrum is that the transit times for these particles are considerably shorter than the rise time of 3.1 h. Thus, the electrons easily populate the¯ux tube to 2.5 AU faster than their rate of injection. On March 23, Ulysses was located at a distance of 2.5 AU from the Sun, and the Ulysses footpoint mapped back to a longitude of ~W60°on the Sun as viewed from the Earth.…”
Section: Discussionmentioning
confidence: 99%
“…Previous observational studies (e.g. Anderson et al 1995;Roelof et al 1992;Bieber et al 2002;Tan et al 2009) have provided evidence of the presence of discrete solar windinterplanetary magnetic field structures beyond 1 AU, which are able to reflect SEPs back to the inner heliosphere. The present study provides another example in which the electron propagation is influenced by a similar structure.…”
Section: Discussionmentioning
confidence: 99%
“…Helios 1 encounters the event near central meridian and observes a peak in the 3-6 MeV proton intensity near the shock passage time. The intensities at the other s/c, after reaching a peak, begin to track closely those seen at Helios 1 after they enter the socalled 'reservoir' region (see also McKibben 1972;Roelof et al 1992) in which the intensities and energy spectra are nearly identical. These results indicate that only a small number of particles can leak out of the reservoir.…”
Section: Multi-spacecraft Observations Of Sep Eventsmentioning
confidence: 65%
“…These results indicate that only a small number of particles can leak out of the reservoir. Observations have provided strong evidence for the location of magnetic 'barriers' in space beyond 1 AU and their role in determining the decay phase of SEP events and the establishment and maintenance of particle reservoirs in the heliosphere (Roelof et al 1992(Roelof et al , 2012aSarris and Malandraki 2003;Tan et al 2012). Reames et al (1996) also considered that the decay phase of the SEP events consists of particles propagating between the converging magnetic field near the Sun and a moving shell of strong scattering formed downstream of the distant traveling shocks.…”
Section: Multi-spacecraft Observations Of Sep Eventsmentioning
confidence: 99%