2025MNRAS.542.2421S


Query : 2025MNRAS.542.2421S

2025MNRAS.542.2421S - Mon. Not. R. Astron. Soc., 542, 2421-2430 (2025/September-3)

Evidence for an intrinsic luminosity-decay correlation in GRB radio afterglows.

SHILLING S.P.R., OATES S.R., KANN D.A., PATEL J., RACUSIN J.L., CENKO B., GUPTA R., SMITH M., RHODES L., HINDS K.R., NICHOLL M., BREEVELD A., PAGE M., DE PASQUALE M. and GOMPERTZ B.

Abstract (from CDS):

We present the discovery of a correlation, in a sample of 16 gamma-ray burst 8.5 GHz radio afterglows, between the intrinsic luminosity measured at 10 d in the rest frame, $L_{\mathrm{Radio,10\,d}}$, and the average rate of decay past this time, $\alpha _{{>}10\,\mathrm{ d}}$. The correlation has a Spearman's rank coefficient of $-0.70 \pm 0.13$ at a significance of ${>}3\sigma$ and a linear regression fit of $\alpha _{>10\,\mathrm{ d}} = -0.29^{+0.19}_{-0.28} \log \left(L_{\mathrm{Radio,10\,d}} \right) + 8.12^{+ 8.86}_{-5.88}$. This finding suggests that more luminous radio afterglows have higher average rates of decay than less luminous ones. We use a Monte Carlo simulation to show the correlation is not produced by chance or selection effects at a confidence level of ${>}3\sigma$. Previous studies found this relation in optical/UV, X-ray, and GeV afterglow light curves, and we have now extended it to radio light curves. The Spearman's rank coefficients and the linear regression slopes for the correlation in each waveband are all consistent within $1\sigma$. We discuss how these new results in the radio band support the effects of observer viewing geometry, and time-varying microphysical parameters, as possible causes of the correlation as suggested in previous works.

Abstract Copyright: © The Author(s) 2025. Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): gamma-ray burst: general

Simbad objects: 21

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Number of rows : 21
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
2 GRB 000911 gB 02 18 42 +07 48.0           ~ 163 0
3 GRB 190114C gB 03 38 01.18 -26 56 47.8           ~ 343 0
4 SN 2016jca SN* 06 06 51.36 -26 47 29.7           SNIc 140 0
5 GRB 970508 gB 06 53 49.2 +79 16 19           ~ 883 1
6 GRB 070125 gB 07 51 17.80 +31 09 04.8           ~ 188 0
7 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 576 0
8 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
9 SN 2017iuk SN* 11 09 39.49 -12 35 18.7           SNII 210 0
10 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
11 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
12 GRB 000418 gB 12 25 21 +20 05.0           ~ 219 0
13 GRB 130907A gB 14 23 34.03 +45 36 27.1           ~ 120 0
14 GRB 010222 G 14 52 12.5 +43 01 06           ~ 364 1
15 GRB 000301C gB 16 20 18.5 +29 26 35           ~ 361 0
16 GRB 991208 gB 16 33 53.51 +46 27 21.5           ~ 269 1
17 GRB 000926 gB 17 04 15 +51 46.0           ~ 373 0
18 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 198 0
19 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
20 GRB 221009A gB 19 13 03.85 +19 46 22.7           ~ 433 0
21 GRB 980703 gB 23 59 06.7 +08 35 07           ~ 453 1

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