2024A&A...692A..73G


Query : 2024A&A...692A..73G

2024A&A...692A..73G - Astronomy and Astrophysics, volume 692A73 (2024/12-1)

Incidence of afterglow plateaus in gamma-ray bursts associated with binary neutron star mergers.

GUGLIELMI L., STRATTA G., DALL'OSSO S., SINGH P., BRUSA M. and PERNA R.

Abstract (from CDS):

One of the most surprising gamma-ray burst (GRB) features discovered with the Swift X-ray telescope (XRT) is a plateau phase in the early X-ray afterglow light curves. These plateaus are observed in the majority of long GRBs, while their incidence in short GRBs (SGRBs) is still uncertain due to their fainter X-ray afterglow luminosity with respect to long GRBs. An accurate estimate of the fraction of SGRBs with plateaus is of utmost relevance given the implications that the plateau may have for our understanding of the jet structure and possibly of the nature of the binary neutron star (BNS) merger remnant. This work presents the results of an extensive data analysis of the largest and most up-to-date sample of SGRBs observed with the XRT, and for which the redshift has been measured. We find a plateau incidence of 18-37% in SGRBs, which is a significantly lower fraction than that measured in long GRBs (> 50%). Although still debated, the plateau phase could be explained as energy injection from the spin-down power of a newly born magnetized neutron star (NS; magnetar). We show that this scenario can nicely reproduce the observed short GRB (SGRBs) plateaus, while at the same time providing a natural explanation for the different plateau fractions between short and long GRBs. In particular, our findings may imply that only a minority of BNS mergers generating SGRBs leave behind a sufficiently stable or long-lived NS to form a plateau. From the probability distribution of the BNS remnant mass, a fraction 18-37% of short GRB plateaus implies a maximum NS mass in the range ∼2.3 - 2.35 M⊙.

Abstract Copyright: © The Authors 2024

Journal keyword(s): equation of state - gamma-ray burst: general - stars: magnetars

Simbad objects: 57

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Number of rows : 57
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 SDSS J002243.71-001657.5 G 00 22 43.71720 -00 16 57.5256           ~ 69 0
2 GRB 140930B gB 00 25 23.40 +24 17 41.7           ~ 52 0
3 GRB 200826A gB 00 27 08.47 +34 01 36.5           ~ 121 0
4 Fermi bn100117879 G 00 45 04.6610 -01 35 42.020           ~ 155 0
5 Fermi bn111117510 gB 00 50 46.220 +23 00 39.22           ~ 141 0
6 GRB 180805B gB 01 43 07.59 -17 29 36.4           ~ 32 0
7 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
8 PSO J047.1631+13.1580 G 03 08 39.14930640 +13 09 29.0253240           ~ 144 0
9 Fermi bn130912358 gB 03 10 25.60 +13 59 55.7           ~ 57 0
10 GRB 200411A gB 03 10 39.39 -52 19 03.3           ~ 31 0
11 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
12 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
13 GRB 170728A gB 03 55 36 +12 10.0           ~ 22 0
14 GRB 060313 G 04 26 28.4020 -10 50 39.901 20.55 21.03 19.66     ~ 156 0
15 Fermi bn161001045 gB 04 47 40.84 -57 15 39.9           ~ 41 0
16 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
17 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
18 GRB 091109B gB 07 30 59.90 -54 05 30.6           ~ 57 0
19 Fermi bn081226044 G 08 02 00.4500 -69 01 49.500           ~ 63 0
20 GRB 160525B G 09 57 32.2460 +51 12 24.600           ~ 30 0
21 GRB 160410A gB 10 02 44.37 +03 28 42.7           ~ 75 0
22 GRB 150424A gB 10 09 13.35 -26 37 51.2           ~ 94 0
23 GRB 121226A G 11 14 34.1210 -30 24 22.840           ~ 44 0
24 GRB 160303A gB 11 14 48.16 +22 44 31.3           ~ 47 0
25 Fermi bn180618030 G 11 19 45.8010 +73 50 15.030           ~ 38 0
26 Fermi bn180418281 G 11 20 29.2100 +24 55 58.734           ~ 57 0
27 GRB 211023B G 11 21 14.3110 +39 08 08.360           ~ 32 0
28 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
29 GALEX J123205.0-105600 Bz? 12 32 04.9717245480 -10 56 00.722548932         16.421 ~ 186 0
30 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
31 GRB 210726A G 12 53 09.8200 +19 11 25.032           ~ 36 0
32 GRB 110402A gB 13 09 36.54 +61 15 10.3           ~ 67 0
33 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
34 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
35 SDSS J140910.47+275320.8 G 14 09 10.47535 +27 53 20.8393           ~ 279 0
36 GRB 060801 G 14 12 01.2620 +16 58 55.970           ~ 172 0
37 GRB 150831A gB 14 44 05.84 -25 38 06.3           ~ 38 0
38 GRB 150423A gB 14 46 18.96 +12 17 00.6           ~ 79 0
39 GRB 120804A G 15 35 47.5100 -28 46 56.110           ~ 99 0
40 Fermi bn170728961 G 15 51 55.5290 +70 07 22.038           ~ 54 0
41 GRB 140903A G 15 52 03.2650 +27 36 10.710           ~ 138 0
42 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
43 GRB 140516A gB 16 51 57.40 +39 57 46.3           ~ 38 0
44 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 190 0
45 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
46 Fermi bn131004904 gB 19 44 27.20 -02 57 31.0           ~ 113 0
47 GRB 140622A gB 21 08 41.56 -14 25 09.5           ~ 61 0
48 Fermi bn210323918 G 21 11 47.3200 +25 22 09.989           ~ 44 0
49 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
50 GRB 140129B G 21 47 01.6490 +26 12 23.270           ~ 30 0
51 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
52 Fermi bn151229285 gB 21 57 28.78 -20 43 55.2           ~ 38 0
53 GRB 110112A gB 21 59 43.77 +26 27 24.4           ~ 47 0
54 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
55 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
56 GRB 191019A gB 22 40 05.87 -17 19 40.8           ~ 55 0
57 GRB 180727A G 23 06 40.0380 -63 03 07.088           ~ 29 0

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