Table 1
Parameters of thermal and non-thermal plasma taken from MHD and test-particle simulations of the reconnecting twisted loops for three different stages.
Stage | nb, | γ | Rfp, | nL, | TL, |
1013m-3 | Mm | 1015 m-3 | MK | ||
|
|||||
Model A, Strong convergence, Bfp = 1180 G | |||||
Onset | 2.9 | 1.7 | 2.0 | 3.2 | 12 |
Fast | 3.0 | 2.1 | 2.2 | 3.8 | 16 |
Decay | 0.12 | 3.7 | 4.1 | 3.4 | 4 |
|
|||||
Model B, Weak convergence, Bfp = 320 G | |||||
Onset | 4.1 | 1.5 | 3.2 | 3.6 | 18 |
Fast | 2.7 | 2.2 | 4.7 | 3.9 | 20 |
Decay | 0.19 | 3.0 | 5.6 | 3.9 | 7 |
|
|||||
Model C, Weak convergence, Bfp = 680 G | |||||
Onset | 8.2 | 1.6 | 3.2 | 3.3 | 30 |
Fast | 4.2 | 2.0 | 4.8 | 3.8 | 36 |
Decay | 0.64 | 3.5 | 5.6 | 3.9 | 15 |
Notes. Here, nb and γ are the non-thermal electron density and power-law index of their energy spectrum. The lower and upper energy cut-offs are 10 keV and 1 MeV, respectively. Parameters nL and TL are the thermal plasma density and temperature within the flaring loop, respectively, and Rfp is the cross-section of the flaring loop near the footpoints.
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