2025ApJ...990L..54L


Query : 2025ApJ...990L..54L

2025ApJ...990L..54L - Astrophys. J., 990, L54 (2025/September-2)

Detection of Low-redshift Excess in Supernova-linked Gamma-Ray Bursts.

LI Q.-M., SUN Q.-B., QIAN S.-B. and LI F.-X.

Abstract (from CDS):

Gamma-ray bursts (GRBs) are traditionally classified into long (lGRBs) and short durations based on their T90, with lGRBs widely used as tracers of the cosmic star formation rate (SFR) due to their observed association with core-collapse supernovae (SNe). However, recent detections of kilonovae accompanying some lGRBs challenge this assumption, suggesting potential contamination from compact binary mergers. Here, we move beyond the conventional T90-based classification and focus exclusively on GRBs directly associated with SNe-the most direct signatures of massive stellar collapse-to reassess their connection to the SFR. Using a sample of SN/GRBs, we construct the luminosity-redshift (L-z) plane and uncover a significant correlation between these variables. To account for observational biases, we apply the τ statistic and Lynden-Bell's C– method to derive the intrinsic luminosity function and formation rate. Our analysis reveals that even among this well-defined subsample, the SN/GRB formation rate still exceeds the SFR at low redshifts (z < 1). These findings suggest that GRBs at low redshift may not serve as reliable tracers of the SFR, and that larger samples are required to further investigate this discrepancy.

Abstract Copyright: © 2025. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Gamma-ray bursts - Star formation - Luminosity function - Supernovae

Simbad objects: 66

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Number of rows : 66
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 101225A gB 00 00 47.48 +44 36 01.0           ~ 163 0
2 GRB 180720B gB 00 02 06.99 -02 55 07.8           ~ 215 0
3 GRB 200826A gB 00 27 08.47 +34 01 36.5           ~ 121 0
4 SN 2010ma SN* 00 48 55.35 -34 33 59.5           SNIc 190 1
5 GRB 050824 gB 00 48 56.100 +22 36 32.00 19.66 21.03 20.46 23.70   ~ 184 0
6 Fermi bn120729456 gB 00 52 17.84 +49 56 23.1           ~ 122 0
7 GRB 041006 gB 00 54 50.17 +01 14 07.0           ~ 202 2
8 SN 2011kl SN* 00 57 22.64 -46 48 03.6           SNSLSN 268 1
9 GRB 040924 gB 02 06 22.52 +16 08 48.8           ~ 169 1
10 GRB 000911 gB 02 18 42 +07 48.0           ~ 163 0
11 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
12 GRB 071112C gB 02 36 50.89 +28 22 16.9           ~ 164 0
13 SN 2013ez SN* 02 53 56.70 +13 23 13.6           ~ 118 0
14 SN 2019oyw SN* 02 58 10.510 -08 57 27.20           ~ 218 0
15 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
16 GRB 190114C gB 03 38 01.18 -26 56 47.8           ~ 343 0
17 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
18 GRB 060904B gB 03 52 50.520 -00 43 30.61 18.27 19.14 18.37     ~ 208 0
19 GRB 230307A gB 04 03 26.24 -75 22 43.8           ~ 221 0
20 GRB 171010A gB 04 26 19.41 -10 27 47.9           SNIc-BL 109 0
21 GRB 211023A gB 04 49 +85.3           ~ 42 0
22 GRB 970228 gB 05 01 46.7 +11 46 53           ~ 650 1
23 Fermi bn141004973 gB 05 06 56.11 +12 49 10.1           ~ 75 0
24 SN 2016jca SN* 06 06 51.36 -26 47 29.7           SNIc 140 0
25 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 303 0
26 SN 2010bh SN* 07 10 30.63 -56 15 19.7           SNIc 336 1
27 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 576 0
28 SN 2002lt SN* 08 08 59.858 +06 43 37.52           SNIc: 363 1
29 GRB 980326 gB 08 36 34.3 -18 51 24           ~ 268 0
30 SN 2012bz SN* 09 07 38.38 +14 01 07.5           SNIb/c 193 1
31 Fermi bn111228657 gB 10 00 16.04 +18 17 52.2           ~ 201 0
32 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
33 SN 2017iuk SN* 11 09 39.49 -12 35 18.7           SNII 210 0
34 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
35 GRB 011121 gB 11 34 26.67 -76 01 41.6       23.0   ~ 286 1
36 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
37 GRB 020305 gB 12 42 27.9 -14 18 12           ~ 45 0
38 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
39 GRB 020405 gB 13 58 03.12 -31 22 22.2   21.9 21.5     ~ 259 1
40 GRB 090429B gB 14 02 40.10 +32 10 14.6           ~ 166 0
41 SDSS J140910.47+275320.8 G 14 09 10.47535 +27 53 20.8393           ~ 279 0
42 SN 2013dx SN* 14 29 14.77 +15 46 26.6           ~ 178 0
43 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
44 GRB 150818A gB 15 21 25.49 +68 20 31.2           ~ 53 0
45 GRB 150518A gB 15 36 48.22 +16 19 47.3           ~ 31 0
46 GRB 991208 gB 16 33 53.51 +46 27 21.5           ~ 269 1
47 GRB 230812B gB 16 36 31.49 +47 51 31.3           ~ 89 0
48 SN 2018fip SN* 16 54 15.64 -54 02 39.5           SNIc-BL 83 0
49 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 198 0
50 Fermi bn140506880 gB 18 27 06.04 -55 38 08.7           ~ 113 0
51 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 400 1
52 GRB 080503 gB 19 06 28.74 +68 47 35.8           ~ 172 0
53 GRB 221009A gB 19 13 03.85 +19 46 22.7           ~ 433 0
54 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
55 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
56 GRB 181201A gB 21 17 11.20 -12 37 50.9           ~ 60 0
57 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
58 GRB 030723 gB 21 49 24.40 -27 42 47.4           ~ 130 0
59 iPTF 14bfu SN* 21 52 30.00 +32 00 52.5           SNIc 80 0
60 GRB 060505 gB 22 07 03.440 -27 48 51.89           ~ 286 1
61 GRB 990712 gB 22 31 53.061 -73 24 28.58           ~ 268 1
62 SN 2008hw SN* 22 39 50.39 -40 08 49.1           SNIc 197 1
63 GRB 020903 gB 22 48 42.34 -20 46 09.3           ~ 248 1
64 GRB 201015A gB 23 37 16.43 +53 24 57.6           ~ 74 0
65 SN 2012eb SN* 23 41 38.35 -46 11 07.0           SNIb/c 62 1
66 SN 2013fu SN* 23 54 29.91 +29 25 47.6           SNIb/c 144 1

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