2022MNRAS.513.1078D


Query : 2022MNRAS.513.1078D

2022MNRAS.513.1078D - Mon. Not. R. Astron. Soc., 513, 1078-1087 (2022/June-2)

A comparative study of luminosity functions and event rate densities of long GRBs with non-parametric method.

DONG X.F., LI X.J., ZHANG Z.B. and ZHANG X.L.

Abstract (from CDS):

In this work, we restudy the dependence of luminosity function and event rates for different gamma-ray burst samples on the criteria of sample selection and threshold effect. To compare with many previous studies, we have chosen two samples including 88 and 118 long bursts with known redshift and peak flux over 2.6 ph cm–2 s–1, from which 79 bursts are picked out to constitute our complete sample. It is found that the evolution of luminosity with redshift can be expressed by L∝(1 + z)k with a diverse k relied more on the sample selection. Interestingly, the cumulative distributions of either non-evolving luminosities or redshifts are found to be also determined by the sample selection rather than the instrumental sensitivity. Nevertheless, the non-evolving luminosities of our samples are similarly distributed with a comparable break luminosity of L0 ∼ 1051 erg s–1. Importantly, we verify with a K-S test that three cases of event rates for the two burst samples evolve with redshift similarly except a small discrepancy due to sampling differences at low-redshift of z < 1, in which all event rates show an excess of Gaussian profile instead of monotonous decline no matter whether the sample is complete. Most importantly, it is found that the burst rates violate the star formation rate at low redshift, while both of them are good in agreement with each other in the higher-redshift regions as many authors discovered previously. Therefore, we predict that two types of long bursts are favored in terms of their associations with both the star formation and the cosmic metallicity.

Abstract Copyright: © 2022 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): methods: data analysis - gamma-ray burst: general - stars: luminosity function, mass function - galaxies: star formation

Simbad objects: 120

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Number of rows : 120
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 bn131231198 gB 00 42 44.0 -01 29 40           ~ 103 0
2 SN 2010ma SN* 00 48 55.35 -34 33 59.5           SNIc 190 1
3 Fermi bn120729456 gB 00 52 17.84 +49 56 23.1           ~ 122 0
4 GRB 081222 gB 01 30 57.76 -34 05 44.0           ~ 199 0
5 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
6 Fermi bn091208410 gB 01 57 38.50 +16 52 50.7           ~ 220 0
7 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
8 GRB 091018 gB 02 08 46 -57 33.0           ~ 169 0
9 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
10 GRB 080411 gB 02 31 54.82 -71 18 07.5           ~ 109 0
11 GRB 050603 gB 02 39 56.839 -25 10 54.92     18.48     ~ 174 0
12 GRB 060306 gB 02 44 22.830 -02 08 55.00           ~ 119 0
13 Fermi bn130925164 gB 02 44 42.38 -26 09 15.8           ~ 184 0
14 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
15 SN 2013ez SN* 02 53 56.70 +13 23 13.6           ~ 118 0
16 Fermi bn100728439 gB 02 56 13.44 +00 16 51.6           ~ 142 0
17 GRB 120802A gB 02 59 22.04 +13 46 05.0           ~ 76 0
18 Fermi bn090926914 gB 03 05 14.30 -38 59 50.9           ~ 149 1
19 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 315 1
20 GRB 050318 gB 03 18 51.000 -46 23 43.61 18.10 18.68 17.58     ~ 189 0
21 GRB 060210 gB 03 50 57.370 +27 01 34.40   20.27       ~ 275 0
22 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
23 GRB 111008A gB 04 01 48.220 -32 42 34.09           ~ 127 0
24 GRB 171010A gB 04 26 19.41 -10 27 47.9           SNIc-BL 109 0
25 Fermi bn120907017 gB 04 58 59.99 -09 18 53.7           ~ 89 0
26 Fermi bn150514774 gB 04 59 30.45 -60 58 07.0           ~ 51 0
27 Fermi bn141004973 gB 05 06 56.11 +12 49 10.1           ~ 75 0
28 Fermi bn100728095 gB 05 55 02.00 -15 15 20.2           ~ 157 0
29 GRB 081121 gB 05 57 07.70 -60 36 42.1           ~ 152 0
30 GRB 090328 gB 06 02 39.69 -41 52 55.1           ~ 194 1
31 SN 2016jca SN* 06 06 51.36 -26 47 29.7           SNIc 140 0
32 GRB 110422A gB 07 28 11.21 +75 06 24.0           ~ 113 0
33 GRB 071020 gB 07 58 39.65 +32 51 38.8           ~ 158 0
34 Fermi bn120119170 gB 08 00 06.940 -09 04 53.83           ~ 193 0
35 GRB 150323A gB 08 32 42.73 +45 27 52.9           ~ 68 0
36 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
37 GRB 130408A gB 08 57 37.30 -32 21 38.9           ~ 98 0
38 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
39 Fermi bn141225959 gB 09 15 06.77 +33 47 30.9           ~ 64 0
40 GRB 130505A gB 09 17 21.9014988888 +01 42 03.426207768           ~ 94 0
41 GRB 061021 gB 09 40 36.120 -21 57 05.40 18.21 19.20 16.82     ~ 160 0
42 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
43 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
44 Fermi bn111228657 gB 10 00 16.04 +18 17 52.2           ~ 201 0
45 GRB 071010B gB 10 02 09.20 +45 43 52.2           ~ 173 0
46 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
47 GRB 110205A gB 10 58 31.12 +67 31 31.2           ~ 213 0
48 GRB 080430 gB 11 01 14.63 +51 41 07.8           ~ 157 0
49 Fermi bn120712571 gB 11 18 21.16 -20 02 01.1           ~ 90 0
50 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
51 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
52 GRB 080603B gB 11 46 07.46 +68 03 38.5           ~ 153 0
53 Fermi bn100615083 gB 11 48 49.25 -19 28 52.2           ~ 133 0
54 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
55 GRB 090424 gB 12 38 07.40 +16 49 45.9           ~ 269 0
56 GRB 080607A gB 12 59 47.14 +15 55 09.6           ~ 257 0
57 Fermi bn121211574 gB 13 02 07.99 +30 08 54.6           ~ 99 0
58 Fermi bn130420313 gB 13 04 25.49 +59 25 26.8           ~ 112 0
59 Fermi bn120811649 gB 13 18 43.82 +62 18 02.8           ~ 113 0
60 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 330 0
61 GRB 150727A gB 13 35 52.52 -18 19 32.7           ~ 59 0
62 GRB 130907A gB 14 23 34.03 +45 36 27.1           ~ 120 0
63 SN 2013dx SN* 14 29 14.77 +15 46 26.6           ~ 178 0
64 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
65 GRB 050802 gB 14 37 05.820 +27 47 12.62 16.85 17.38 16.97     ~ 186 0
66 GRB 060814 gB 14 45 21.480 +20 35 11.80           ~ 241 0
67 Fermi bn160804065 gB 14 46 31.20 +09 59 56.1           ~ 79 0
68 Fermi bn130610133 gB 14 57 40.91 +28 12 25.8           ~ 89 0
69 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 180 0
70 GRB 081203A gB 15 32 07.6 +63 31 15           ~ 177 0
71 Fermi bn120922939 gB 15 38 59.67 -20 10 55.0           ~ 88 0
72 GRB 110715A gB 15 50 44.090 -46 14 06.53           ~ 120 0
73 Fermi bn101213451 gB 16 05 15.27 +21 53 50.5           ~ 68 0
74 GRB 070521 gB 16 10 38.600 +30 15 22.70           ~ 164 0
75 GRB 120327A gB 16 27 27.49 -29 24 53.8           ~ 116 0
76 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
77 GRB 090715B gB 16 45 21.59 +44 50 20.1           ~ 144 0
78 GRB 091003A gB 16 46 04.680 +36 37 31.08           ~ 135 0
79 Fermi bn170903534 gB 16 58 06.22 +34 58 44.6           ~ 42 0
80 GRB 140508A gB 17 01 51.95 +46 46 49.5           ~ 76 0
81 GRB 080319C gB 17 15 55.48 +55 23 31.7           ~ 174 0
82 Fermi bn130612141 gB 17 19 10.63 +16 43 11.8           ~ 89 0
83 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 198 0
84 Fermi bn151027166 gB 18 09 56.87 +61 21 12.3           ~ 143 0
85 Fermi bn120326056 gB 18 15 37.06 +69 15 35.4           ~ 188 0
86 GRB 120909A gB 18 22 56.81 -59 26 54.9           ~ 103 0
87 Fermi bn140506880 gB 18 27 06.04 -55 38 08.7           ~ 113 0
88 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 400 1
89 GRB 160425A gB 18 41 18.56 -54 21 36.1           ~ 49 0
90 Fermi bn110731465 gB 18 42 00.99 -28 32 13.8           ~ 193 0
91 GRB 080413A gB 19 09 11.73 -27 40 39.6           ~ 163 0
92 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
93 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
94 GRB 130514A gB 19 45 07.33 -07 58 41.1           ~ 82 0
95 Fermi bn121128212 gB 20 02 23.88 +54 17 59.1           ~ 128 0
96 GRB 071003 gB 20 07 24.50 +10 56 48.8           ~ 181 0
97 GRB 070508 gB 20 51 11.810 -78 23 04.88     19.62     ~ 144 0
98 GRB 160623A gB 21 01 11.54 +42 13 15.5           ~ 73 0
99 GRB 100621A gB 21 01 13.12 -51 06 22.5           ~ 204 0
100 Fermi bn161129300 gB 21 04 54.66 +32 08 05.5           ~ 65 0
101 Fermi bn110818860 gB 21 09 20.890 -63 58 51.80           ~ 92 0
102 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
103 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
104 iPTF 14bfu SN* 21 52 30.00 +32 00 52.5           SNIc 80 0
105 Fermi bn080804972 gB 21 54 41.90 -53 11 20.2           ~ 158 0
106 GRB 060927A gB 21 58 11.930 +05 21 50.32           ~ 215 0
107 GRB 051109A gB 22 01 15.320 +40 49 23.70   20.09 20.14     ~ 190 0
108 GRB 071117 gB 22 20 10.40 -63 26 36.6           ~ 112 0
109 Fermi bn080916406 gB 22 25 09.30 -57 01 33.7           ~ 177 0
110 GRB 151001B gB 22 27 21.27 +64 41 39.1           ~ 16 0
111 Fermi bn091024380 gB 22 37 +56.9           ~ 151 0
112 SN 2008hw SN* 22 39 50.39 -40 08 49.1           SNIc 197 1
113 Fermi bn150821406 gB 22 47 39.15 -57 53 38.2           ~ 71 0
114 GRB 131030A gB 23 00 16.14 -05 22 05.2           ~ 126 0
115 GRB 051111A gB 23 12 33.170 +18 22 28.80 19.77 20.08 19.50     ~ 223 0
116 Fermi bn100816026 gB 23 26 57.56 +26 34 42.6           ~ 170 0
117 GRB 090812 gB 23 32 48.5 -10 36 17           ~ 165 0
118 GRB 130701A gB 23 48 55.05 +36 06 01.2           ~ 81 0
119 GRB 061222A gB 23 53 03.419 +46 31 58.60           ~ 177 0
120 SN 2013fu SN* 23 54 29.91 +29 25 47.6           SNIb/c 144 1

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