2024A&A...686A..56K


Query : 2024A&A...686A..56K

2024A&A...686A..56K - Astronomy and Astrophysics, volume 686A56 (2024/6-1)

Fires in the deep: The luminosity distribution of early-time gamma-ray-burst afterglows in light of the Gamow Explorer sensitivity requirements.

KANN D.A., WHITE N.E., GHIRLANDA G., OATES S.R., MELANDRI A., JELINEK M., DE UGARTE POSTIGO A., LEVAN A.J., MARTIN-CARRILLO A., PAEK G.S.-H., IZZO L., BLAZEK M., THONE C.C., AGUI FERNANDEZ J.F., SALVATERRA R., TANVIR N.R., CHANG T.-C., O'BRIEN P., ROSSI A., PERLEY D.A., IM M., MALESANI D.B., ANTONELLI A., COVINO S., CHOI C., D'AVANZO P., D'ELIA V., DICHIARA S., FAUSEY H.M., FUGAZZA D., GOMBOC A., GORSKI K.M., GRANOT J., GUIDORZI C., HANLON L., HARTMANN D.H., HUDEC R., JUN H.D., KIM J., KIM Y., KLOSE S., KLUZNIAK W., KOBAYASHI S., KOUVELIOTOU C., LIDZ A., MARONGIU M., MARTONE R., MEINTJES P., MUNDELL C.G., MURPHY D., NALEWAJKO K., PARK W.-K., SZECSI D., SMITH R.J., STECKLUM B., STEELE I.A., STROBL J., SUNG H.-I.-, UPDIKE A., URATA Y. and VAN DER HORST A.J.

Abstract (from CDS):

Context. Gamma-ray bursts (GRBs) are ideal probes of the Universe at high redshift (ɀ), pinpointing the locations of the earliest star-forming galaxies and providing bright backlights with simple featureless power-law spectra that can be used to spectrally fingerprint the intergalactic medium and host galaxy during the period of reionization. Future missions such as Gamow Explorer (hereafter Gamow) are being proposed to unlock this potential by increasing the rate of identification of high-ɀ (ɀ > 5) GRBs in order to rapidly trigger observations from 6 to 10 m ground telescopes, the James Webb Space Telescope (JWST), and the upcoming Extremely Large Telescopes (ELTs).
Aims. Gamow was proposed to the NASA 2021 Medium-Class Explorer (MIDEX) program as a fast-slewing satellite featuring a wide-field lobster-eye X-ray telescope (LEXT) to detect and localize GRBs with arcminute accuracy, and a narrow-field multi-channel photo-ɀ infrared telescope (PIRT) to measure their photometric redshifts for > 80% of the LEXT detections using the Lyman-α dropout technique. We use a large sample of observed GRB afterglows to derive the PIRT sensitivity requirement.
Methods. We compiled a complete sample of GRB optical-near-infrared (optical-NIR) afterglows from 2008 to 2021, adding a total of 66 new afterglows to our earlier sample, including all known high-ɀ GRB afterglows. This sample is expanded with over 2837 unpublished data points for 40 of these GRBs. We performed full light-curve and spectral-energy-distribution analyses of these after-glows to derive their true luminosity at very early times. We compared the high-ɀ sample to the comparison sample at lower redshifts. For all the light curves, where possible, we determined the brightness at the time of the initial finding chart of Gamow, at different high redshifts and in different NIR bands. This was validated using a theoretical approach to predicting the afterglow brightness. We then followed the evolution of the luminosity to predict requirements for ground- and space-based follow-up. Finally, we discuss the potential biases between known GRB afterglow samples and those to be detected by Gamow.
Results. We find that the luminosity distribution of high-ɀ GRB afterglows is comparable to those at lower redshift, and we therefore are able to use the afterglows of lower-ɀ GRBs as proxies for those at high ɀ. We find that a PIRT sensitivity of 15 µJy (21 mag AB) in a 500 s exposure simultaneously in five NIR bands within 1000 s of the GRB trigger will meet the Gamow mission requirements. Depending on the ɀ and NIR band, we find that between 75% and 85% of all afterglows at ɀ > 5 will be recovered by Gamow at 5σ detection significance, allowing the determination of a robust photo-ɀ. As a check for possible observational biases and selection effects, we compared the results with those obtained through population-synthesis models, and find them to be consistent.
Conclusions. Gamow and other high-ɀ GRB missions will be capable of using a relatively modest 0.3 m onboard NIR photo-ɀ telescope to rapidly identify and report high-ɀ GRBs for further follow-up by larger facilities, opening a new window onto the era of reionization and the high-redshift Universe.

Abstract Copyright: © The Authors 2024

Journal keyword(s): methods: observational - space vehicles - space vehicles: instruments - techniques: photometric - gamma-ray burst: general - dark ages, reionization, first stars

VizieR on-line data: <Available at CDS (J/A+A/686/A56): sources.dat tableb1.dat>

Simbad objects: 101

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Number of rows : 101
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 180720B gB 00 02 06.99 -02 55 07.8           ~ 215 0
2 GRB 070110 gB 00 03 39.270 -52 58 27.00 21.8 21.9 21.2     ~ 220 0
3 GRB 150910A gB 00 22 40.14 +33 28 22.4           ~ 79 0
4 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
5 SN 2010ma SN* 00 48 55.35 -34 33 59.5           SNIc 190 1
6 Fermi bn120729456 gB 00 52 17.84 +49 56 23.1           ~ 122 0
7 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
8 GRB 050904 gB 00 54 50.794 +14 05 09.42           ~ 496 0
9 SN 2011kl SN* 00 57 22.64 -46 48 03.6           SNSLSN 268 1
10 GRB 201014A gB 01 23 11.09 +27 39 36.9           ~ 18 0
11 Fermi bn100814160 gB 01 29 53.61 -17 59 43.6           ~ 219 0
12 GRB 100901A gB 01 49 03.56 +22 45 30.6           ~ 170 0
13 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
14 Fermi bn091208410 gB 01 57 38.50 +16 52 50.7           ~ 220 0
15 GRB 100905A gB 02 06 12.06 +14 55 45.9           ~ 45 0
16 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
17 GRB 091018 gB 02 08 46 -57 33.0           ~ 169 0
18 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
19 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
20 GRB 140801A gB 02 56 16.50 +30 56 16.8           ~ 55 0
21 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
22 GRB 190114C gB 03 38 01.18 -26 56 47.8           ~ 343 0
23 SN 2019jrj SN* 03 38 01.190 -26 56 46.77           ~ 10 0
24 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 168 0
25 GRB 080913 gB 04 22 57.90 -25 07 38.6           ~ 213 0
26 GRB 121024A gB 04 41 53.31 -12 17 26.1           ~ 143 0
27 GRB 151027B gB 05 04 52.67 -06 27 00.7           ~ 61 0
28 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
29 GRB 060116 gB 05 38 46.170 -05 26 15.08           ~ 86 0
30 Fermi bn150301818 gB 05 56 40.04 -57 58 10.4           ~ 67 0
31 SN 2016jca SN* 06 06 51.36 -26 47 29.7           SNIc 140 0
32 GRB 000131 gB 06 13 31.08 -51 56 41.7     24.7     ~ 172 1
33 Fermi bn120711115 gB 06 18 42.839 -70 59 56.78           ~ 125 0
34 Fermi bn080928628 gB 06 20 16.85 -55 11 59.3           ~ 187 0
35 GRB 140430A gB 06 51 44.58 +23 01 25.5           ~ 81 0
36 GRB 110422A gB 07 28 11.21 +75 06 24.0           ~ 113 0
37 Fermi bn120119170 gB 08 00 06.940 -09 04 53.83           ~ 193 0
38 SN 2002lt SN* 08 08 59.858 +06 43 37.52           SNIc: 363 1
39 GRB 140419A gB 08 27 57.56 +46 14 25.3           ~ 95 0
40 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
41 GRB 100205A gB 09 25 33.00 +31 44 25.8           ~ 39 0
42 GRB 160327A gB 09 46 48.56 +54 00 46.4           ~ 43 0
43 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
44 Fermi bn111228657 gB 10 00 16.04 +18 17 52.2           ~ 201 0
45 GRB 100219A gB 10 16 48.48 -12 34 00.0           ~ 130 0
46 GRB 210312B gB 10 23 22.3 +76 52 17           ~ 7 0
47 GRB 180325A gB 10 29 42.57 +24 27 48.7           ~ 85 0
48 GRB 110205A gB 10 58 31.12 +67 31 31.2           ~ 213 0
49 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
50 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
51 GRB 080603B gB 11 46 07.46 +68 03 38.5           ~ 153 0
52 GRB 140515A gB 12 24 15.48 +15 06 17.7           ~ 90 0
53 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
54 [OBV2016] GN-z11 EmG 12 36 25.46 +62 14 31.4           ~ 247 0
55 GRB 080607A gB 12 59 47.14 +15 55 09.6           ~ 257 0
56 Fermi bn140423356 gB 13 09 06.20 +49 50 18.3           ~ 114 0
57 Fermi bn141221338 gB 13 13 09.02 +08 12 18.3           ~ 76 0
58 GRB 140311A gB 13 57 13.29 +00 38 31.7           ~ 86 0
59 GRB 090429B gB 14 02 40.10 +32 10 14.6           ~ 166 0
60 GRB 120521C gB 14 17 09.10 +42 08 39.8           ~ 93 0
61 GRB 201221A gB 14 17 55.22 -45 24 58.2           ~ 28 0
62 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
63 GRB 130606B gB 14 34 07.04 -22 06 08.2           ~ 47 0
64 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 180 0
65 GRB 990123 gB 15 25 29 +44 45.0     8.95     ~ 1012 1
66 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
67 GRB 081203A gB 15 32 07.6 +63 31 15           ~ 177 0
68 GRB 120404A gB 15 40 02.29 +12 53 06.3           ~ 104 0
69 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 389 0
70 GRB 110715A gB 15 50 44.090 -46 14 06.53           ~ 120 0
71 GRB 120327A gB 16 27 27.49 -29 24 53.8           ~ 116 0
72 GRB 090726 gB 16 34 43.50 +72 51 56.5           ~ 70 0
73 GRB 140629A gB 16 35 54.44 +41 52 36.7           ~ 89 0
74 GRB 130606A gB 16 37 35.12 +29 47 46.4           ~ 185 0
75 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 198 0
76 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 198 0
77 Fermi bn120326056 gB 18 15 37.06 +69 15 35.4           ~ 188 0
78 GRB 120815A gB 18 15 54.40 -52 07 29.0           ~ 103 0
79 Fermi bn140506880 gB 18 27 06.04 -55 38 08.7           ~ 113 0
80 GRB 080603A gB 18 37 37.95 +62 44 39.6           ~ 89 0
81 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 224 0
82 Fermi bn110731465 gB 18 42 00.99 -28 32 13.8           ~ 193 0
83 GRB 110726A gB 19 06 52.21 +56 04 16.4           ~ 55 0
84 GRB 080413A gB 19 09 11.73 -27 40 39.6           ~ 163 0
85 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
86 GRB 120923A gB 20 15 10.73 +06 13 16.9           ~ 59 0
87 GRB 160625B gB 20 34 23.67 +06 55 11.1           ~ 235 0
88 GRB 210905A gB 20 36 11.64 -44 26 24.3           ~ 42 0
89 GRB 161023A gB 20 44 05.20 -47 39 48.7           ~ 49 0
90 GRB 100621A gB 21 01 13.12 -51 06 22.5           ~ 204 0
91 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
92 GRB 181201A gB 21 17 11.20 -12 37 50.9           ~ 60 0
93 GRB 060522 gB 21 31 44.850 +02 53 10.80           ~ 140 0
94 GRB 080413B gB 21 44 34.62 -19 58 51.2           ~ 191 0
95 Fermi bn091024380 gB 22 37 +56.9           ~ 151 0
96 SN 2008hw SN* 22 39 50.39 -40 08 49.1           SNIc 197 1
97 GRB 131030A gB 23 00 16.14 -05 22 05.2           ~ 126 0
98 GRB 081029 gB 23 07 06 -68 10.7           ~ 121 0
99 GRB 071025 gB 23 40 17.02 +31 46 42.4           ~ 122 0
100 SN 2012eb SN* 23 41 38.35 -46 11 07.0           SNIb/c 62 1
101 SN 2013fu SN* 23 54 29.91 +29 25 47.6           SNIb/c 144 1

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