2025A&A...702A.173Z


Query : 2025A&A...702A.173Z

2025A&A...702A.173Z - Astronomy and Astrophysics, volume 702A173 (2025/10-1)

Unsupervised machine learning classification of gamma-ray bursts based on the rest-frame prompt emission parameters.

ZHU S.-Y., SHAO L., TAM P.-H.T. and ZHANG F.-W.

Abstract (from CDS):

Gamma-ray bursts (GRBs) are generally believed to originate from two distinct progenitors, namely, compact binary mergers and massive collapsars. Traditional methods, along with a number of recent machine learning-based classification schemes, predominantly rely on observer-frame physical parameters, which are significantly affected by the redshift effects and might not accurately represent the intrinsic properties of GRBs. In particular, the progenitors could typically only be determined on the basis of a successful detection of the multiband long-term afterglow, which could easily cost days of devoted effort from multiple global observational utilities. In this work, we applied the unsupervised machine learning (ML) algorithms t-SNE and UMAP to perform the GRB classification based on rest-frame prompt emission parameters. The map results of both t-SNE and UMAP reveal a clear division of these GRBs into two clusters, denoted as GRBs-I and GRBs-II. We find that all supernova-associated GRBs, including the atypical short-duration burst GRB 200826A (now recognized as collapsar-origin), consistently fall within the GRBs-II category. Conversely, all kilonova-associated GRBs (except for two controversial events) are classified as GRBs-I, including the peculiar long-duration burst GRB 060614 originating from a merger event. In another words, this clear ML separation of two types of GRBs based only on prompt properties could correctly predict the results of progenitors without follow-up afterglow properties. A comparative analysis with conventional classification methods using T90 and E_p, z_-Eiso correlation demonstrates that our machine learning approach provides superior discriminative power, particularly with respect to resolving ambiguous cases of hybrid GRBs.

Abstract Copyright: © The Authors 2025

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

VizieR on-line data: <Available at CDS (J/A+A/702/A173): tablea2.dat>

Status at CDS : Tables of objects will be appraised for possible ingestion in SIMBAD.

Simbad objects: 89

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Number of rows : 89
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 220101A gB 00 05 24.89 +31 46 07.7           ~ 85 0
2 GRB 140930B gB 00 25 23.40 +24 17 41.7           ~ 52 0
3 Fermi bn180703876 gB 00 25 52.72 -67 10 47.9           ~ 35 0
4 GRB 200826A gB 00 27 08.47 +34 01 36.5           ~ 121 0
5 GRB 200415A gB 00 47 30.0 -25 11 37           ~ 70 0
6 NGC 253 SyG 00 47 33.134 -25 17 19.68   8.03   6.94 8.1 ~ 3588 2
7 GRB 180128A gB 00 49 -26.1           ~ 12 0
8 GRB 201021C gB 00 50 06.93 -55 51 55.8           ~ 21 0
9 NAME Sculptor Dwarf Galaxy G 01 00 09.4 -33 42 32   9.79 8.6 8.81   ~ 1498 4
10 GRB 201216C gB 01 05 28.88 +16 30 58.0           ~ 89 0
11 GRB 221226B gB 01 31 38.07 -41 31 36.0           ~ 15 0
12 GRB 180805B gB 01 43 07.59 -17 29 36.4           ~ 32 0
13 GRB 210722A gB 01 48 07.26 -06 20 51.3           ~ 31 0
14 GRB 040924 gB 02 06 22.52 +16 08 48.8           ~ 169 1
15 GRB 201103B gB 02 48 44.29 +12 08 18.9           ~ 24 0
16 GRB 191011A gB 02 58 54.70 -27 50 43.4           ~ 38 0
17 GRB 191004B gB 03 16 48.97 -39 38 06.3           ~ 32 0
18 GRB 190324A gB 03 18 27.77 -47 12 54.1           ~ 35 0
19 GRB 181010A gB 03 30 16.88 -23 02 17.9           ~ 39 0
20 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
21 GRB 230307A gB 04 03 26.24 -75 22 43.8           ~ 221 0
22 Fermi bn161001045 gB 04 47 40.84 -57 15 39.9           ~ 41 0
23 GRB 211023A gB 04 49 +85.3           ~ 42 0
24 Fermi bn150514774 gB 04 59 30.45 -60 58 07.0           ~ 51 0
25 GRB 201020B gB 05 01 52.03 +77 04 05.9           ~ 34 0
26 GRB 220117A gB 06 06 17.40 -28 26 14.6           ~ 27 0
27 Fermi bn180314030 gB 06 37 03.66 -24 29 46.5           ~ 46 0
28 GRB 210104A gB 06 55 05.38 +64 40 34.1           ~ 53 0
29 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
30 GRB 210204A gB 07 48 19.37 +11 24 34.2           ~ 46 0
31 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 576 0
32 SN 2002lt SN* 08 08 59.858 +06 43 37.52           SNIc: 363 1
33 GRB 240225B gB 08 33 27.10 +27 04 28.5           ~ 21 0
34 GRB 231115A gB 08 43.0 +73 30           ~ 59 0
35 GRB 211227A gB 08 48 35.73 -02 44 07.1           ~ 57 0
36 M 82 AGN 09 55 52.430 +69 40 46.93 9.61 9.30 8.41     ~ 6156 6
37 GRB 200613A gB 10 12 10.03 +45 45 14.1           ~ 36 0
38 GRB 191221B gB 10 19 19.17 -38 09 27.5           ~ 66 0
39 GRB 240315C gB 10 37 22.0 +10 50 04           ~ 21 0
40 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
41 GRB 240218A gB 10 47 11.24 +01 16 34.8           ~ 27 0
42 SN 2017iuk SN* 11 09 39.49 -12 35 18.7           SNII 210 0
43 GRB 210702A gB 11 14 18.89 -36 44 49.8           ~ 40 0
44 GRB 220107A gB 11 19 13.68 +34 10 14.3           ~ 29 0
45 Fermi bn180618030 G 11 19 45.8010 +73 50 15.030           ~ 38 0
46 GRB 201221D gB 11 24 14.19 +42 08 35.5           ~ 48 0
47 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
48 Fermi bn130716442 gB 11 58 17.69 +63 03 11.6           ~ 27 0
49 GRB 190613A gB 12 10 07.13 +67 14 07.0           ~ 26 0
50 GRB 240414A gB 12 19 08.10 +56 44 26.0           ~ 3 0
51 GALEX J123205.0-105600 Bz? 12 32 04.9717245480 -10 56 00.722548932         16.421 ~ 186 0
52 GRB 110402A gB 13 09 36.54 +61 15 10.3           ~ 67 0
53 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
54 GRB 230204B gB 13 10 34.60 -21 43 00.8           ~ 28 0
55 GRB 220627A gB 13 25 28.51 -32 25 34.5           ~ 31 0
56 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
57 GRB 210610A gB 13 37 07.74 +14 27 55.4           ~ 43 0
58 SDSS J140910.47+275320.8 G 14 09 10.47535 +27 53 20.8393           ~ 279 0
59 GRB 200524A gB 14 12 10.74 +60 54 19.4           ~ 40 0
60 GRB 201221A gB 14 17 55.22 -45 24 58.2           ~ 28 0
61 GRB 150831A gB 14 44 05.84 -25 38 06.3           ~ 38 0
62 Fermi bn170728961 G 15 51 55.5290 +70 07 22.038           ~ 54 0
63 GRB 190719C gB 16 00 49.50 +13 00 00.6           ~ 43 0
64 GRB 220219B gB 16 03 39.39 +31 14 02.5           ~ 11 0
65 GRB 210610B gB 16 15 40.47 +14 23 56.3           ~ 87 0
66 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
67 GRB 230812B gB 16 36 31.49 +47 51 31.3           ~ 89 0
68 GRB 210210A gB 17 31 04.90 +14 39 45.1           ~ 30 0
69 GRB 220521A gB 18 20 55.15 +10 22 18.4           ~ 38 0
70 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 190 0
71 Fermi bn110731465 gB 18 42 00.99 -28 32 13.8           ~ 193 0
72 GRB 230818A gB 19 03 33.15 +40 53 48.2           ~ 37 0
73 PSO J285.9246+45.7134 G 19 03 41.90914320 +45 42 48.4220520           ~ 63 0
74 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
75 Fermi bn131004904 gB 19 44 27.20 -02 57 31.0           ~ 113 0
76 GRB 210731A gB 20 01 13.13 -28 03 39.7           ~ 28 0
77 GRB 210822A gB 20 17 44.99 +05 17 00.5           ~ 49 0
78 Fermi bn210323918 G 21 11 47.3200 +25 22 09.989           ~ 44 0
79 GRB 210619B gB 21 18 52.39 +33 51 00.2           ~ 93 0
80 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
81 GRB 220527A gB 21 34 06.70 +14 58 18.7           ~ 27 0
82 GRB 231117A gB 22 09 37.00 +13 30 58.1           ~ 54 0
83 NVSS J230126-385839 rG 23 01 26.7650 -38 58 40.422   22.22 21.22 21   ~ 325 1
84 GRB 240205B gB 23 25 52 -55 07.4           ~ 21 0
85 Fermi bn100816026 gB 23 26 57.56 +26 34 42.6           ~ 170 0
86 GRB 201015A gB 23 37 16.43 +53 24 57.6           ~ 74 0
87 GRB 231210B gB ~ ~           ~ 17 0
88 GRB 231118A gB ~ ~           ~ 27 0
89 GRB 131203A gB ~ ~           ~ 2 0

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