2020ApJ...902...82S


Query : 2020ApJ...902...82S

2020ApJ...902...82S - Astrophys. J., 902, 82-82 (2020/October-2)

A late-time radio Survey of short gamma-ray bursts at z < 0.5: new constraints on the remnants of neutron-star mergers.

SCHROEDER G., MARGALIT B., FONG W.-F., METZGER B.D., WILLIAMS P.K.G., PATERSON K., ALEXANDER K.D., LASKAR T., GOYAL A.V. and BERGER E.

Abstract (from CDS):

Massive, rapidly spinning magnetar remnants produced as a result of binary neutron-star (BNS) mergers may deposit a fraction of their energy into the surrounding kilonova ejecta, powering a synchrotron radio signal from the interaction of the ejecta with the circumburst medium. Here, we present 6.0 GHz Very Large Array (VLA) observations of nine, low-redshift short gamma-ray bursts (GRBs; z < 0.5) on rest-frame timescales of ≃2.4-13.9 yr following the bursts. We place 3σ limits on radio continuum emission of Fν <= 6-20 µJy at the burst positions, or Lν <= (0.6-8.3) x 1028 erg s–1 Hz–1. Comparing these limits with new light-curve modeling that properly incorporates relativistic effects, we obtain limits on the energy deposited into the ejecta of Eej <= (0.6-6.7) x 1052 erg (Eej≲(1.8–17.6)×1052 erg) for an ejecta mass of 0.03 M☉ (0.1 M☉). We present a uniform reanalysis of 27 short GRBs with 5.5-6.0 GHz observations, and find that >=50% of short GRBs did not form stable magnetar remnants in their mergers. Assuming short GRBs are produced by BNS mergers drawn from the Galactic BNS population plus an additional component of high-mass GW194025-like mergers in a fraction fGW190425 of cases, we place constraints on the maximum mass of a nonrotating neutron star (NS; Tolman-Oppenheimer-Volkoff mass; MTOV), finding MTOV≲2.23M☉ for fGW190425 = 0.4; this limit increases for larger values of fGW190425. The detection (or lack thereof) of radio remnants in untargeted surveys such as the VLA Sky Survey (VLASS) could provide more stringent constraints on the fraction of mergers that produce stable remnants. If ≳30–300 radio remnants are discovered in VLASS, this suggests that short GRBs are a biased population of BNS mergers in terms of the stability of the remnants they produce.

Abstract Copyright: © 2020. The American Astronomical Society. All rights reserved.

Journal keyword(s): Gamma-ray bursts - Magnetars - Neutron stars

Simbad objects: 34

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Number of rows : 34
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 Fermi bn150120123 G 00 41 16.5630 +33 59 42.598           ~ 70 0
2 Fermi bn100117879 G 00 45 04.6610 -01 35 42.020           ~ 155 0
3 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2924 2
4 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
5 GRB 130822A gB 01 51 41.27 -03 12 31.7           ~ 34 0
6 PSO J047.1631+13.1580 G 03 08 39.14930640 +13 09 29.0253240           ~ 144 0
7 GRB 070729 gB 03 45 16.04 -39 19 19.9           ~ 81 0
8 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
9 ICRF J054236.1+495107 Sy1 05 42 36.13789710 +49 51 07.2337139   18.45 17.80 17.210   ~ 1573 1
10 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
11 PSR J0740+6620 Psr 07 40 45.799 +66 20 33.60           ~ 395 0
12 SDSS J093805.33+153719.0 G 09 38 05.33384 +15 37 19.0406           ~ 146 0
13 GRB 150424A gB 10 09 13.35 -26 37 51.2           ~ 94 0
14 GRB 090515 gB 10 56 41.0 +14 27 22           ~ 122 0
15 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
16 SDSS J123612.87+285858.8 BiC 12 36 12.8803407000 +28 58 58.780075656           ~ 328 1
17 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
18 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
19 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
20 GRB 140903A G 15 52 03.2650 +27 36 10.710           ~ 138 0
21 NVSS J155207+273501 rG 15 52 07.8735967464 +27 35 01.661612568           ~ 6 0
22 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
23 GRB 060502B gB 18 35 46.060 +52 37 51.45           ~ 153 1
24 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 190 0
25 Fermi bn130515056 gB 18 53 45.65 -54 16 45.0           ~ 55 0
26 PSO J285.9246+45.7134 G 19 03 41.90914320 +45 42 48.4220520           ~ 63 0
27 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
28 Fermi bn090621922 gB 20 53 49.30 +69 02 02.9           ~ 65 0
29 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
30 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
31 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
32 GRB 080123 gB 22 35 46.100 -64 54 03.24           ~ 98 0
33 Fermi bn100816026 gB 23 26 57.56 +26 34 42.6           ~ 170 0
34 GRB 190425 GWE ~ ~           ~ 438 0

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