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Table 2.

Best-fit values of the magnetar magnetic field strength B and initial spin period P for the 13 out of 15 cases for which the magnetar model fit of the luminosity light curve is successful.

GRB name Input Output

z θj B P τ sd 680 ( P ms B 15 ) 2 $ \tau_{\mathrm{sd}} \approx 680 \left(\frac{P_{\mathrm{ms}}}{B_{15}}\right)^2 $ χ2 ν
(deg) (1014 G) (ms) (ks)
051221A 0.5464 6.0 (29 ± 2) (12.8 ± 0.3) 13.3 ± 2.1 125 77
060614 0.125 12.6 (37 ± 3) (24 ± 1) 34 ± 9 1749 465
070714B 0.923 8.6 (132 ± 40) (11 ± 2) 0.5 ± 0.3 284 79
090510 0.903 2.3 (82 ± 7) (4.5 ± 0.2) 0.20 ± 0.04 80 63
110402A 0.854 15.0 (96 ± 37) (14 ± 1) 1.4 ± 1.1 42.0 16
130603B 0.3568 6.3 (110 ± 2) (13.2 ± 0.2) 0.98 ± 0.04 137 70
140903A 0.3529 4.0 (32 ± 4) (8 ± 0.3) 4.5 ± 1.2 56 36
150424A 0.3 4.3 (36 ± 4) (16 ± 1) 13 ± 3 243 115
151229A 0.63 5.0 (67 ± 9) (4.3 ± 0.9) 0.3 ± 0.1 142 56
161001A 0.67 5.0 (47 ± 6) (4.2 ± 0.2) 0.5 ± 0.1 88 54
170728B 1.272 3.5 (20 ± 1) (1.50 ± 0.03) 0.39 ± 0.04 232 193
210323A 0.733 2.9 (51 ± 11) (8.7 ± 0.6) 2.0 ± 0.9 62 18
211211A 0.0763 6.9 (286 ± 26) (27 ± 1) 0.6 ± 0.1 779 265

Notes. Besides the redshift z and the jet half-opening angle θj of each SGRB, the table also shows the spin-down timescale τsd implied by B and P (see e.g. Dall’Osso & Stella 2022), as well as the fit χ2 and degrees of freedom ν.

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