Open Access

Table B.1.

Number of major solar wind plasma types and the fraction of each type in anticorrelated structures in different groups.

N major plasma type a $ N_{\text{ major~plasma~type}}^{\mathrm{a}} $ One Two Three Four
5 (4)b 8 (8) 3 (4) 0 (0)
32 (30) 35 (32) 19 (24) 1 (1)
19 (19) 29 (24) 15 (19) 0 (1)
18 (15) 14 (16) 7 (9) 1 (0)
Nmajor plasma type = 1 streamer-belt-origin coronal-hole-origin sector-reversal-region ejecta
0 (0) 0 (0) 0 (0) 5 (4)
19 (20) 10 (8) 2 (1) 1 (1)
10 (11) 6 (6) 2 (1) 1 (1)
9 (9) 4 (2) 0 (0) 5 (4)
Nmajor plasma type > 2c streamer-belt-origin coronal-hole-origin sector-reversal-region ejecta Number of cases
36.8% (30.4%) 3.6% (6.0%) 12.4% (14.0%) 47.2% (49.7%) 3(4)
34.8% (35.4%) 14.5% (13.4%) 14.8% (17.3%) 35.9% (33.8%) 20(25)
32.8% (34.79%) 13.1% (13.5%) 14.0% (13.7%) 38.1% (25.2%) 15(20)
39.3% (34.7%) 13.1% (9.9%) 15.3% (24.0%) 32.2% (31.4%) 8(9)
non-ICME&Fe-up 32.8%(34.0%) 13.1%(13.6%) 14.0%(14.4%) 40.2%(38.0%) 15(19)
non-ICME&Fe-down 40.8%(39.8%) 18.8%(12.8%) 17.1%(26.7%) 23.2%(20.7%) 5(6)
ICMEs in 2001d 17.0% 6.5% 21.4% 55.1% -
Solar wind in 2001e 49.5% 15.8% 20.6% 14.1% -
Solar wind in 2007e 35.8% 26.3% 34.4% 3.5% -

a If the proportion of one solar wind type is over 10%, it is considered as a major type. Solar wind types are based on the four-plasma categorization scheme from Xu & Borovsky (2015).

b The values outside the brackets are based on Sstrong (corresponding to solid markers), and the values within the brackets are based on Sweak (corresponding to empty markers).

c A relatively remarkable mixture of plasma from different origins is very likely.

d ICMEs from Cane & Richardson (2003), calculations are based on 12-min averaged solar wind plasma data.

e Based on 12-min averaged solar wind plasma data, ICMEs excluded.

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