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Table 4

Best-fit results from FM90 model fits to the afterglow SEDs of 24 GRBs, all of which were best-fitted by a broken-power model in our initial SED analysis (see Table 1).

GRB Local-dusta Power Law αx ~ αo
model E(B − V) χ2/d.o.f. c 1 E(B − V) χ2/d.o.f. (Y/N)

050319 mw 58/78 62/78 Y
050820A lmc 0.06 ± 0.01 177/143 2.95 ± 0.25 0.23 ± 0.05 190/143 N
060206 mw  <0.08 61/59  <0.03 84/59 N
060418 smc 19/23  <0.01 29/23 N
060729 smc 0.05 ± 0.01 176/191  <0.15 180/191 Y
061121 lmc 87/93 86/93 N
061126 lmc 170/140 0.36 ± 0.05 168/140 N
070110 smc  <0.07 129/112 137/112 Y
080210 lmc 0.08 ± 0.01 23/25 0.09 ± 0.02 35/25 N
080411 mw  <0.02 81/83 b 0.00 216/83 Y
080413B mw 78/69 75/69 Y
080430 smc  <0.07 38/40 52/40 Y
080721 mw 0.13 ± 0.05 168/153 0.77 ± 0.06 168/153 N
080804 lmc 0.033 ± 0.004 38/42 b  <0.01 92/42 N
080916A smc 0.21 ± 0.05 18/26 19/26 N
081121 smc 52/47 b  <0.01 92/47 N
081203A mw 0.09 ± 0.01 76/80 0.23 ± 0.05 61/80 Y
081222 mw 34/46 b  <0.01 155/46 N
090102 mw 0.13 ± 0.01 22/27 0.16 ± 0.02 35/27 N
090424 mw 0.37 ± 0.03 92/83 0.52 ± 0.08 95/83 Y
090618 smc 24/18  <3.7  <0.02 36/18 Y
091018 smc 0.033 ± 0.005 55/52 b 0.00 101/52 N
091029 lmc 0.02 ± 0.01 23/23 b  <0.02 58/23 Y
091127 lmc  <0.01 186/173 b 0.00 326/173 N

Notes. All FM90 model parameters were fixed to the best-fit values from the simultaneous SED analysis (see Table 3) apart from the coefficient c1, which determines the slope of the extinction curve. Column 8 indicates whether the optical and X-ray light curve decay rates are consistent (Y) or not (N) at epoch of the corresponding GRB afterglow SED. Those GRBs better fit by a single power-law spectral component and an FM90 host extinction curve are highlighted in bold (see text for details).

(a)

The best-fit local dust model when using the broken power-law model, chosen from the mean SMC (smc), LMC (lmc) and Milky Way (mw) extinction laws.

(b)

c1 is unconstrained.

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