1994
DOI: 10.1086/191887
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Energetic-particle abundances in impulsive solar flare events

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Cited by 252 publications
(205 citation statements)
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“…The plateau in the Fe/O curve seen on the right side of Figures 3È5, and to some extent in the 22Ne/20Ne and Fe/Mg curves in Figure 6, is consistent with the earlier results of Mason et al (1986) and Reames et al (1994), who found no correlation with Fe enrichments and 3He/4He for 3He/4He [ 0.1. It appears that for the impulsive events, the 3He/4He can change by orders of magnitude without a corresponding change in the other abundances.…”
Section: Observationssupporting
confidence: 91%
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“…The plateau in the Fe/O curve seen on the right side of Figures 3È5, and to some extent in the 22Ne/20Ne and Fe/Mg curves in Figure 6, is consistent with the earlier results of Mason et al (1986) and Reames et al (1994), who found no correlation with Fe enrichments and 3He/4He for 3He/4He [ 0.1. It appears that for the impulsive events, the 3He/4He can change by orders of magnitude without a corresponding change in the other abundances.…”
Section: Observationssupporting
confidence: 91%
“…For impulsive events, associated with Ñares, the average abundances also show a trend in Q/A, with smaller Q/A values having larger enhancements, but they do not typically follow a power law. Furthermore, for some SEP events, the 3He/4He ratio is observed to be enhanced by as much as a factor of 104 compared with the solar wind values of 4.8 ] 10~4 (Ogilvie et al 1980 ;Hsieh & Simpson 1970 ;Reames, von Rosenvinge, & Lin 1985 ;Reames, Meyer, & von Rosenvinge 1994 ;Mason, Dwyer, & Mazur 2000). The enhancement of 3He does not follow the same pattern as the heavier elements, since the Q/A for 3He and 4He would predict a 3He depletion, rather than an enhancement.…”
Section: Introductionmentioning
confidence: 86%
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“…When electron acceleration ceases, the 3 He/ 4 He ratio is frozen and no further ion acceleration occurs. The time-integrated total number of 3 He nuclei being accelerated above 1.3 MeV amu À1 in an impulsive flare is about 10 31 particles (Reames et al 1994). Assuming the flaring area to be of about 10 17 cm 2 with a scale height of 10 9 cm, the proton density n H ¼ 5 Â 10 10 cm À3 , and 3 He=H ¼ 5 Â 10 À5 , there are 2:5 Â 10 32 3 He ions available in the flaring volume.…”
Section: Abundance Enhancementsmentioning
confidence: 99%
“…3. A time-integrated total of about 10 31 3 He nuclei is required to account for the observed particle fluxes (Reames, Meyer, & von Rosenvinge 1994).…”
Section: No 1 2003mentioning
confidence: 99%