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Table 3.
Inverse solutions for multiple observers, using the 1D and 2D SEP propagator models.
| Energy | Rigidity | λ∥ | λ⊥ | λ⊥/λ∥ | Injection | Injection | ta | te | RSTA2 | RSolO2 | REarth2 | Rmean2 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|
| (MeV) | (MV) | (AU) | (AU) | (%) | source (°) | time (UT) | (hours) | (hours) | (%) | (%) | (%) | (%) |
| Electrons | ||||||||||||
| 0.115 | 0.361 | 0.14 | 0.0014 | 1 | 20 | 2021-10-28 15:17 | 0.8 | 1.8 | 98 | 96 | 92 | 95 |
| 0.180 | 0.463 | 0.14 | 0.0013 | 0.9 | 20 | 2021-10-28 15:20 | 0.8 | 1.4 | 98 | 95 | 91 | 95 |
| 0.314 | 0.647 | 0.13 | 0.0021 | 1.5 | 15 | 2021-10-28 15:24 | 0.8 | 1.0 | 97 | 95 | 97 | 96 |
| 0.400 | 0.752 | 0.13 | 0.0021 | 1.5 | 15 | 2021-10-28 15:23 | 0.8 | 1.0 | 97 | 92 | 88 | 92 |
| 1.0 | 1.4 | 0.12 | 0.0034 | 2.8 | 5 | 2021-10-28 15:19 | 1.6 | 0.4 | 93 | 96 | 95 | |
| 2.5 | 2.46 | 0.12 | 0.0036 | 3 | 5 | 2021-10-28 15:18 | 1.8 | 0.4 | 95 | 98 | 91 | 95 |
| Protons | ||||||||||||
| 108 | 463 | 0.26 | 0.0117 | 4.5 | 20 | 2021-10-28 15:33 | 1.6 | 2.1 | 95 | 90 | 92 | |
| 130 | 511 | 0.22 | 0.0198 | 9 | 5 | 2021-10-28 15:23 | 1.6 | 1.6 | 99 | 83 | 91 | |
| 300 | 808 | 0.18 | 0.018 | 10 | 5 | 2021-10-28 15:23 | 1.5 | 0.8 | 98 | 98 | ||
| 896 | 1576 | 0.25 | 0.025 | 10 | 5 | 2021-10-28 15:28 | 1.7 | 0.6 | 96 | 96 | ||
Notes. For each species and energy (rigidity) we provide λ∥, λ⊥, and their ratio λ⊥/λ∥; the size of injection source, injection time, acceleration time (ta), and escape time (te); and the R2 scores of the best fits.
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