Table 1
Results of the Gaussian process regression.
ν | S 0 | S m | t m | t r | t d | |
(GHz) | (Jy) | (Jy) | (MJD) | (d) | (d) | |
|
||||||
2.64 | 0.868 | 0.593 ± 0.032 | 55 095.2 | 239.9 | 366.8 | |
4.85 | 0.777 | 1.084 ± 0.031 | 55 016.8 | 201.8 | 383.2 | |
8.35 | 0.740 | 1.764 ± 0.043 | 54 980.4 | 230.9 | 435.9 | |
10.45 | 0.725 | 2.055 ± 0.062 | 54 968.7 | 234.9 | 435.0 | |
14.60 | 0.683 | 2.414 ± 0.088 | 54 954.4 | 288.1 | 467.6 | |
15.00 | 0.711 | 2.570 ± 0.026 | 54 952.3 | 276.2 | 391.7 | |
23.05 | 0.478 | 2.856 ± 0.189 | 54 921.9 | 390.8 | 457.0 | |
32.00 | 0.516 | 2.590 ± 0.277 | 54 916.7 | 447.9 | 446.5 | |
43.05 | 0.299 | 3.542 ± 0.454 | 54 925.8 | 383.4 | 527.2 | |
86.24 | 0.507 | 2.439 ± 0.144 | 54 912.8 | 331.3 | 437.2 | |
142.33 | 0.263 | 1.987 ± 0.254 | 54 888.0 | 313.5 | 444.5 | |
226.50 | 0.238 | 1.823 ± 0.102 | 54 914.3 | 300.3 | 460.8 |
Notes. Columns: (1) observing frequency; (2) minimum flux density subtracted prior to the fit; (3) flare amplitude; (4) time of flare maximum; (5) flare rising time; and (6) decay time. An uncertainty due to temporal resolution of up to 0.3 d can be expected for tm, yielding an uncertainty of about 0.4 d for tr and td.
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