2022ApJ...935...16E


Query : 2022ApJ...935...16E

2022ApJ...935...16E - Astrophys. J., 935, 16 (2022/August-2)

Extragalactic Millimeter Transients in the Era of Next-generation CMB Surveys.

EFTEKHARI T., BERGER E., METZGER B.D., LASKAR T., VILLAR V.A., ALEXANDER K.D., HOLDER G.P., VIEIRA J.D., WHITEHORN N. and WILLIAMS P.K.G.

Abstract (from CDS):

The next generation of wide-field cosmic microwave background (CMB) surveys are uniquely poised to open a new window into time-domain astronomy in the millimeter band. Here, we explore the discovery phase space for extragalactic transients with near-term and future CMB experiments to characterize the expected population. We use existing millimeter-band light curves of known transients (gamma-ray bursts, tidal disruption events, fast blue optical transients (FBOTs), neutron star mergers) and theoretical models, in conjunction with known and estimated volumetric rates. Using Monte Carlo simulations of various CMB survey designs (area, cadence, depth, duration) we estimate the detection rates and the resulting light-curve characteristics. We find that existing and near-term surveys will find tens to hundreds of long-duration gamma-ray bursts (LGRBs), driven primarily by detections of the reverse shock emission, and including off-axis LGRBs. Next-generation experiments (CMB-S4, CMB-HD) will find tens of FBOTs in the nearby universe and will detect a few tidal disruption events. CMB-HD will additionally detect a small number of short gamma-ray bursts, where these will be discovered within the detection volume of next-generation gravitational wave experiments like the Cosmic Explorer.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Radio transient sources - Radio sources - Transient sources - Transient detection - Gamma-ray astronomy - Gamma-ray bursts

Simbad objects: 58

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Number of rows : 58
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 041219 gB 00 24 27.7 +62 50 34           ~ 231 1
3 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
4 Fermi bn131231198 gB 00 42 44.0 -01 29 40           ~ 103 0
5 GRB 050904 gB 00 54 50.794 +14 05 09.42           ~ 496 0
6 Fermi bn140304557 gB 02 02 33.90 +33 28 27.9           ~ 106 0
7 SN 2013ez SN* 02 53 56.70 +13 23 13.6           ~ 118 0
8 SN 2019oyw SN* 02 58 10.510 -08 57 27.20           ~ 218 0
9 GRB 190114C gB 03 38 01.18 -26 56 47.8           ~ 343 0
10 GRB 060904B gB 03 52 50.520 -00 43 30.61 18.27 19.14 18.37     ~ 208 0
11 SN 2016jca SN* 06 06 51.36 -26 47 29.7           SNIc 140 0
12 GRB 970508 gB 06 53 49.2 +79 16 19           ~ 883 1
13 GRB 080129 gB 07 01 08.13 -07 50 47.8           ~ 85 0
14 GRB 980329 gB 07 02 41 +38 50.7           ~ 276 1
15 GRB 070125 gB 07 51 17.80 +31 09 04.8           ~ 188 0
16 SN 2013ak SN* 08 07 06.69 -28 03 10.1           SNII 22 0
17 SN 2008D SN* 09 09 30.625 +33 08 20.16     17.5     SNIb 458 1
18 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
19 SN 1993J SN* 09 55 24.77476 +69 01 13.7026   10.8 12.0     SNIIb 1507 1
20 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
21 GRB 130418A gB 09 56 08.86 +13 40 01.8           ~ 70 0
22 GRB 191221B gB 10 19 19.17 -38 09 27.5           ~ 66 0
23 GRB 131108A gB 10 26 00.480 +09 39 44.05           ~ 96 0
24 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
25 SN 2017iuk SN* 11 09 39.49 -12 35 18.7           SNII 210 0
26 GRB 210702A gB 11 14 18.89 -36 44 49.8           ~ 40 0
27 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
28 SN 2020oi SN* 12 22 54.930 +15 49 24.96           SNIc 77 0
29 IGR J12580+0134 gam 12 58 05.1 +01 34 26           ~ 50 0
30 GRB 090313 gB 13 13 36.00 +08 05 10.7           ~ 149 0
31 PTF 11qcj SN* 13 13 41.51 +47 17 57.0           SNIb 62 0
32 SN 2011dh SN* 13 30 05.10555 +47 10 10.9227           SNIIb 445 1
33 AT 2022cmc ev 13 34 43.207 +33 13 00.54           ~ 79 0
34 GRB 140311A gB 13 57 13.29 +00 38 31.7           ~ 86 0
35 SN 2013dx SN* 14 29 14.77 +15 46 26.6           ~ 178 0
36 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
37 iPTF 13bvn SN* 15 00 00.152 +01 52 53.17           SNIb 211 0
38 GRB 110715A gB 15 50 44.090 -46 14 06.53           ~ 120 0
39 GRB 090404 gB 15 56 55.80 +35 31 03.4           ~ 79 0
40 GRB 210610B gB 16 15 40.47 +14 23 56.3           ~ 87 0
41 SN 2018cow SN* 16 16 00.254 +22 16 05.10           SNIb 305 0
42 GRB 000301C gB 16 20 18.5 +29 26 35           ~ 361 0
43 GRB 991208 gB 16 33 53.51 +46 27 21.5           ~ 269 1
44 SWIFT J164449.3+573451 G 16 44 47.81184000 +57 35 00.7113480           ~ 533 0
45 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 198 0
46 Fermi bn120326056 gB 18 15 37.06 +69 15 35.4           ~ 188 0
47 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
48 GRB 071003 gB 20 07 24.50 +10 56 48.8           ~ 181 0
49 GRB 210905A gB 20 36 11.64 -44 26 24.3           ~ 42 0
50 GRB 161023A gB 20 44 05.20 -47 39 48.7           ~ 49 0
51 2MASX J20570298+1412165 G 20 57 02.9650698480 +14 12 16.295014080           ~ 162 0
52 GRB 160623A gB 21 01 11.54 +42 13 15.5           ~ 73 0
53 GRB 100621A gB 21 01 13.12 -51 06 22.5           ~ 204 0
54 GRB 181201A gB 21 17 11.20 -12 37 50.9           ~ 60 0
55 GRB 210619B gB 21 18 52.39 +33 51 00.2           ~ 93 0
56 AT 2020xnd ev 22 20 02.030 -02 50 25.30           ~ 66 0
57 SN 2014C SN* 22 37 05.60 +34 24 31.9           SNIb 167 1
58 GRB 051022A gB 23 56 04.200 +19 36 32.30           ~ 194 1

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