2024ApJ...961..195L


Query : 2024ApJ...961..195L

2024ApJ...961..195L - Astrophys. J., 961, 195 (2024/February-1)

Accessing the Host Galaxies of Long Gamma-Ray Bursts with Next-generation Telescopes.

LAN G.-X., LI Y. and LI Z.

Abstract (from CDS):

We present a method to estimate the detection expectations of host galaxies of long gamma-ray bursts (LGRBs) in the grizJHKL bands. It is found that given the same limiting magnitude ${m}_{{grizJHKL},\mathrm{lim}}$ in each band, the z band produces the largest number of overall LGRB hosts and low-mass hosts (M* ≤ 108M⊙) at ${m}_{{grizJHKL},\mathrm{lim}}\gtrsim 26$ mag. For the detection of high-redshift LGRB hosts (redshift ≥5), it is recommended to prioritize the L band, due to its good performance at both low and high limiting magnitudes. We specifically estimate the expectation of LGRB host detection with ${m}_{{grizJHKL},\mathrm{lim}}=28$ mag, which the James Webb Space Telescope can partially attain. We find that there may exist 116, 259, 277, 439, 266, 294, 274, and 316 LGRB hosts, including 0.54, 31, 28, 143, 12, 20, 14, and 35 low-mass ones in the grizJHKL bands and 13, 14, 15, 14, and 15 high-redshift ones in the zJHKL bands, for 15 yr Swift LGRBs with S ≥ 10–6 erg cm–2. The results show that the study of LGRB hosts under next-generation observational conditions holds significant potential, especially for low-mass host studies. However, it appears that the deeper sensitivities of galaxy telescopes may not significantly enhance statistical studies of high-redshift hosts. Strategies aimed at increasing the number of distant LGRB hosts may require the expansion of high-redshift LGRB detections.

Abstract Copyright: © 2024. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Gamma-ray bursts - Galaxies - Stellar mass functions

Simbad objects: 31

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Number of rows : 31
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 200826A gB 00 27 08.47 +34 01 36.5           ~ 121 0
2 GRB 060202 gB 02 23 22.940 +38 23 03.70           ~ 102 0
3 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
4 GRB 070802 gB 02 27 35.91 -55 31 39.1           ~ 168 0
5 GRB 230307A gB 04 03 26.24 -75 22 43.8           ~ 221 0
6 GRB 080517 gB 06 48 58.00 +50 44 06.3           ~ 52 1
7 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 576 0
8 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
9 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
10 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
11 GRB 050219 gB 11 05 39.03 -40 41 00.8           ~ 11 0
12 Fermi bn120624933 gB 11 23 31.98 +08 55 42.1           ~ 100 0
13 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
14 GRB 011121 gB 11 34 26.67 -76 01 41.6       23.0   ~ 286 1
15 GRB 060319 gB 11 45 33.050 +60 00 39.61 20.10         ~ 73 0
16 GRB 161108A gB 12 03 09.10 +24 52 05.5           ~ 46 0
17 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
18 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 244 1
19 GRB 051008 gB 13 31 28.100 +42 08 05.01 17.06   14.11     ~ 90 0
20 GRB 090417B gB 13 58 44.8 +47 00 55           ~ 119 1
21 SDSS J140910.47+275320.8 G 14 09 10.47535 +27 53 20.8393           ~ 279 0
22 SN 2013dx SN* 14 29 14.77 +15 46 26.6           ~ 178 0
23 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 198 0
24 Fermi bn140506880 gB 18 27 06.04 -55 38 08.7           ~ 113 0
25 GRB 080805 gB 20 56 55.30 -62 25 58.8           ~ 102 0
26 GRB 100621A gB 21 01 13.12 -51 06 22.5           ~ 204 0
27 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
28 Fermi bn081109293 gB 22 03 11.50 -54 42 40.5           ~ 125 1
29 GRB 990712 gB 22 31 53.061 -73 24 28.58           ~ 268 1
30 GRB 061222 gB 23 53.0 +46 32           ~ 18 0
31 GRB 051022A gB 23 56 04.200 +19 36 32.30           ~ 194 1

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