2020A&A...643A.113A


Query : 2020A&A...643A.113A

2020A&A...643A.113A - Astronomy and Astrophysics, volume 643A, 113-113 (2020/11-1)

Observational constraints on the optical and near-infrared emission from the neutron star-black hole binary merger candidate S190814bv.

ACKLEY K., AMATI L., BARBIERI C., BAUER F.E., BENETTI S., BERNARDINI M.G., BHIROMBHAKDI K., BOTTICELLA M.T., BRANCHESI M., BROCATO E., BRUUN S.H., BULLA M., CAMPANA S., CAPPELLARO E., CASTRO-TIRADO A.J., CHAMBERS K.C., CHATY S., CHEN T.-W., CIOLFI R., COLEIRO A., COPPERWHEAT C.M., COVINO S., CUTTER R., D'AMMANDO F., D'AVANZO P., DE CESARE G., D'ELIA V., DELLA VALLE M., DENNEAU L., DE PASQUALE M., DHILLON V.S., DYER M.J., ELIAS-ROSA N., EVANS P.A., EYLES-FERRIS R.A.J., FIORE A., FRASER M., FRUCHTER A.S., FYNBO J.P.U., GALBANY L., GALL C., GALLOWAY D.K., GETMAN F.I., GHIRLANDA G., GILLANDERS J.H., GOMBOC A., GOMPERTZ B.P., GONZALEZ-FERNANDEZ C., GONZALEZ-GAITAN S., GRADO A., GRECO G., GROMADZKI M., GROOT P.J., GUTIERREZ C.P., HEIKKILA T., HEINTZ K.E., HJORTH J., HU Y.-D., HUBER M.E., INSERRA C., IZZO L., JAPELJ J., JERKSTRAND A., JIN Z.P., JONKER P.G., KANKARE E., KANN D.A., KENNEDY M., KIM S., KLOSE S., KOOL E.C., KOTAK R., KUNCARAYAKTI H., LAMB G.P., LELOUDAS G., LEVAN A.J., LONGO F., LOWE T.B., LYMAN J.D., MAGNIER E., MAGUIRE K., MAIORANO E., MANDEL I., MAPELLI M., MATTILA S., McBRIEN O.R., MELANDRI A., MICHALOWSKI M.J., MILVANG-JENSEN B., MORAN S., NICASTRO L., NICHOLL M., NICUESA GUELBENZU A., NUTTAL L., OATES S.R., O'BRIEN P.T., ONORI F., PALAZZI E., PATRICELLI B., PEREGO A., TORRES M.A.P., PERLEY D.A., PIAN E., PIGNATA G., PIRANOMONTE S., POSHYACHINDA S., POSSENTI A., PUMO M.L., QUIROLA-VASQUEZ J., RAGOSTA F., RAMSAY G., RAU A., REST A., REYNOLDS T.M., ROSETTI S.S., ROSSI A., ROSSWOG S., SABHA N.B., SAGUES CARRACEDO A., SALAFIA O.S., SALMON L., SALVATERRA R., SAVAGLIO S., SBORDONE L., SCHADY P., SCHIPANI P., SCHULTZ A.S.B., SCHWEYER T., SMARTT S.J., SMITH K.W., SMITH M., SOLLERMAN J., SRIVASTAV S., STANWAY E.R., STARLING R.L.C., STEEGHS D., STRATTA G., STUBBS C.W., TANVIR N.R., TESTA V., THRANE E., TONRY J.L., TURATTO M., ULACZYK K., VAN DER HORST A.J., VERGANI S.D., WALTON N.A., WATSON D., WIERSEMA K., WIIK K., WYRZYKOWSKI L., YANG S., YI S.-X. and YOUNG D.R.

Abstract (from CDS):


Context. Gravitational wave (GW) astronomy has rapidly reached maturity, becoming a fundamental observing window for modern astrophysics. The coalescences of a few tens of black hole (BH) binaries have been detected, while the number of events possibly including a neutron star (NS) is still limited to a few. On 2019 August 14, the LIGO and Virgo interferometers detected a high-significance event labelled S190814bv. A preliminary analysis of the GW data suggests that the event was likely due to the merger of a compact binary system formed by a BH and a NS.
Aims. In this paper, we present our extensive search campaign aimed at uncovering the potential optical and near infrared electromagnetic counterpart of S190814bv. We found no convincing electromagnetic counterpart in our data. We therefore use our non-detection to place limits on the properties of the putative outflows that could have been produced by the binary during and after the merger.
Methods. Thanks to the three-detector observation of S190814bv, and given the characteristics of the signal, the LIGO and Virgo Collaborations delivered a relatively narrow localisation in low latency - a 50% (90%) credible area of 5deg2 (23deg2) - despite the relatively large distance of 267±52Mpc. ElectromagNetic counterparts of GRAvitational wave sources at the VEry Large Telescope collaboration members carried out an intensive multi-epoch, multi-instrument observational campaign to identify the possible optical and near infrared counterpart of the event. In addition, the ATLAS, GOTO, GRAWITA-VST, Pan-STARRS, and VINROUGE projects also carried out a search on this event. In this paper, we describe the combined observational campaign of these groups.
Results. Our observations allow us to place limits on the presence of any counterpart and discuss the implications for the kilonova (KN), which was possibly generated by this NS-BH merger, and for the strategy of future searches. The typical depth of our wide-field observations, which cover most of the projected sky localisation probability (up to 99.8%, depending on the night and filter considered), is r∼22 (resp. K∼21) in the optical (resp. near infrared). We reach deeper limits in a subset of our galaxy-targeted observations, which cover a total ∼50% of the galaxy-mass-weighted localisation probability. Altogether, our observations allow us to exclude a KN with large ejecta mass M≥0.1M to a high (>90%) confidence, and we can exclude much smaller masses in a sub-sample of our observations. This disfavours the tidal disruption of the neutron star during the merger.
Conclusions. Despite the sensitive instruments involved in the campaign, given the distance of S190814bv, we could not reach sufficiently deep limits to constrain a KN comparable in luminosity to AT 2017gfo on a large fraction of the localisation probability. This suggests that future (likely common) events at a few hundred megaparsecs will be detected only by large facilities with both a high sensitivity and large field of view. Galaxy-targeted observations can reach the needed depth over a relevant portion of the localisation probability with a smaller investment of resources, but the number of galaxies to be targeted in order to get a fairly complete coverage is large, even in the case of a localisation as good as that of this event.

Abstract Copyright: © K. Ackley et al. 2020

Journal keyword(s): gravitational waves - stars: neutron - supernovae: general

VizieR on-line data: <Available at CDS (J/A+A/643/A113): objects.dat photps1.dat>

Simbad objects: 144

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Number of rows : 144
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023
#notes
1 ESO 540-13 G 00 40 58.2514916472 -22 04 59.028148128   15.41   14.31   ~ 10 0
2 AT 2019npe ev 00 41 33.330 -23 44 31.95           ~ 1 0
3 2MASX J00423338-2251587 G 00 42 33.3958174488 -22 51 58.449035880   15.98       ~ 11 0
4 MCG-04-02-039 BiC 00 42 42.3395619624 -21 46 27.199179732   15   13.13   ~ 9 0
5 AT 2019nxd ev 00 42 44.598 -24 57 20.34           ~ 2 0
6 AT 2019mbq SN* 00 43 20.493 -25 53 02.07           SNII 4 0
7 AT 2019nsm ev 00 43 30.160 -22 43 29.35           ~ 2 0
8 LEDA 795185 G 00 43 33.2 -23 57 11           ~ 2 0
9 AT 2019qby ev 00 44 14.334 -25 07 44.32           ~ 1 0
10 6dFGS gJ004448.5-220700 G 00 44 48.4 -22 07 00   16.14   14.72   ~ 5 0
11 2MASX J00445054-2309325 G 00 44 50.5603186584 -23 09 32.901106824   16.43   15.24   ~ 3 0
12 IC 1581 G 00 45 46.307 -25 55 12.69   16.24   15.20   ~ 9 0
13 AT 2019qca ev 00 45 48.540 -26 49 39.01           ~ 1 0
14 2MASX J00455329-2346208 G 00 45 53.3302641576 -23 46 20.578648116   16.28       ~ 6 0
15 AT 2019odc ev 00 46 01.689 -25 27 32.94           ~ 3 0
16 2MASX J00461041-2439006 G 00 46 10.3883909424 -24 39 00.875076768   16.25 16.5     ~ 9 0
17 AT 2019nxe SN* 00 46 16.814 -24 22 21.19           SNIa 4 0
18 AT 2019qcb ev 00 46 19.062 -26 08 43.19           ~ 1 0
19 LEDA 805757 G 00 46 52.9 -23 02 01           ~ 3 0
20 AT 2019npd ev 00 46 56.711 -25 22 36.43           ~ 3 0
21 AT 2019nbp SN? 00 46 57.386 -24 21 42.30           ~ 3 0
22 AT 2019nyv ev 00 46 59.451 -23 05 59.50           ~ 1 0
23 2MASX J00470525-2414193 G 00 47 05.2835562840 -24 14 19.731339492   16.83   15.91   ~ 5 0
24 ESO 474-26 G 00 47 07.5377265072 -24 22 14.800438812   14.51 15.7 13.54   ~ 50 0
25 AT 2019nzr ev 00 47 21.410 -24 34 36.58           ~ 2 0
26 AT 2019okr ev 00 47 23.696 -25 27 30.78           ~ 2 0
27 AT 2019onj ev 00 47 26.006 -25 26 55.13           ~ 2 0
28 AT 2019tih SN? 00 47 26.661 -27 36 03.01           ~ 2 0
29 6dFGS gJ004729.0-252626 G 00 47 28.9713529704 -25 26 25.894466088   16.15   15.27   ~ 6 0
30 NGC 253 SyG 00 47 33.134 -25 17 19.68   8.03   6.94 8.1 ~ 3221 2
31 AT 2019thm SN? 00 47 56.625 -26 54 02.80           ~ 2 0
32 AT 2019ntm ev 00 48 04.398 -23 47 50.94           ~ 2 0
33 AT 2019nyy SN? 00 48 16.650 -26 38 26.92           ~ 2 0
34 2MASX J00482185-2507365 G 00 48 21.8356236192 -25 07 36.771294720   16.29   15.10   ~ 10 1
35 LEDA 3235517 G 00 48 24.7612551000 -25 35 45.113601768   17.202 15.60 15.996   ~ 6 0
36 ESO 540-29 G 00 48 28.9972041552 -22 08 50.806337964   15.36   14.69   ~ 7 0
37 AT 2019nts ev 00 48 31.441 -23 06 40.80           ~ 2 0
38 AT 2019paw SN? 00 48 34.285 -25 05 25.90           ~ 2 0
39 6dFGS gJ004842.0-232207 G 00 48 41.9513469576 -23 22 07.344527628   16.75   15.63   ~ 6 0
40 LEDA 797191 G 00 48 42.8 -23 46 23           ~ 4 0
41 IC 1587 G 00 48 43.3156968744 -23 33 41.910799896   15.57   13.97   ~ 16 0
42 AT 2019tix SN? 00 48 45.678 -24 38 50.59           ~ 2 0
43 PSST 19epf SN* 00 48 47.882 -25 18 23.46           SNII 5 0
44 2MASX J00485495-2504100 G 00 48 54.95280 -25 04 10.0960           ~ 3 0
45 AT 2019omw ev 00 48 56.255 -23 10 12.49           ~ 4 0
46 LEDA 133702 G 00 48 58.3473314592 -25 41 37.437927684   15.846 15.99 14.958   ~ 8 0
47 MCG-04-03-016 G 00 49 01.4983525704 -23 48 40.846313988   15.96       ~ 6 0
48 AT 2019nuj SN? 00 49 01.738 -23 14 04.93           ~ 3 0
49 2dFGRS TGS143Z311 G 00 49 16.8350566176 -26 13 08.932031328   16.182 14.68 14.885   ~ 9 0
50 2MASX J00491968-2628350 G 00 49 19.6733419800 -26 28 34.695828084   16.99 16.80     ~ 6 0
51 2dFGRS TGS143Z307 G 00 49 23.0885079552 -26 30 27.476416584   16.779 15.32 15.438   ~ 7 0
52 2dFGRS TGS143Z303 G 00 49 27.5455455672 -26 32 17.873246868   15.508 14.13 14.825   ~ 11 0
53 2dFGRS TGS143Z297 G 00 49 32.5585821408 -26 32 19.500342144   16.801 16.36 15.788   ~ 6 0
54 AT 2019tii SN? 00 49 35.213 -27 02 09.33           ~ 2 0
55 2dFGRS TGS143Z288 G 00 49 46.0173785640 -26 26 34.426146480   16.041 15.29 15.053   ~ 7 0
56 2dFGRS TGS143Z286 G 00 49 52.2 -25 56 46   17.479   16.630   ~ 5 0
57 2MASX J00495354-2442259 G 00 49 53.5716417960 -24 42 26.392301640   17.12   15.87   ~ 5 0
58 AT 2019mwp ev 00 50 02.820 -22 41 18.78           ~ 1 0
59 2MASX J00500970-2316481 G 00 50 09.7415949216 -23 16 48.462745620   16.47   15.24   ~ 8 0
60 AT 2019ntp ev 00 50 12.072 -26 11 52.56           ~ 5 0
61 AT 2019nme ev 00 50 32.558 -22 13 33.70           ~ 4 0
62 2MASX J00503308-2317437 G 00 50 33.1267468944 -23 17 43.687957992           ~ 5 0
63 2MASX J00503450-2337067 G 00 50 34.5095914632 -23 37 06.585802068   16.62   15.43   ~ 7 0
64 2MASX J00503987-2648482 G 00 50 39.8755736688 -26 48 48.091521492   14.64 14.39     ~ 10 0
65 6dFGS gJ005043.2-225318 G 00 50 43.1615142120 -22 53 18.117391272   16.61   15.47   ~ 5 0
66 2dFGRS TGS143Z088 G 00 50 52.4 -25 34 37   17.599   17.028   ~ 6 0
67 LEDA 798818 G 00 50 54.4 -23 37 55           ~ 5 0
68 IC 1588 G 00 50 57.7181813736 -23 33 28.505172132   16.37   15.05   ~ 9 0
69 AT 2019qbu ev 00 51 09.173 -22 17 40.69           ~ 1 0
70 2MASX J00511052-2557150 G 00 51 10.5050703240 -25 57 14.496021684   16.827 15.48 15.532   ~ 7 0
71 2MASX J00511221-2618470 G 00 51 12.2107623168 -26 18 46.797892776   17.052 16.00 15.805   ~ 7 0
72 6dFGS gJ005114.6-231730 G 00 51 14.5 -23 17 30   17.37   16.03   ~ 3 0
73 2dFGRS TGS143Z250 G 00 51 15.8 -25 57 39   18.035   17.216   ~ 6 0
74 2dFGRS TGS143Z251 G 00 51 18.7352769624 -26 10 04.736720100   17.25 15.88 15.570   ~ 10 0
75 AT 2019nmd ev 00 51 29.004 -22 28 16.96           ~ 4 0
76 LEDA 787700 G 00 51 29.8 -24 38 32           ~ 4 0
77 2MASX J00513144-2604379 G 00 51 31.4156775792 -26 04 37.994456352   17.380   16.407   ~ 5 0
78 2MASX J00521536-2441554 G 00 52 15.3641665248 -24 41 55.188490128   17.27   15.95   ~ 5 0
79 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 10683 1
80 ESO 474-35 G 00 52 41.582 -25 44 01.87   16.86 16.76 15.44   ~ 15 0
81 AT 2019nva ev 00 52 43.339 -23 37 53.64           ~ 1 0
82 NGC 288 GlC 00 52 45.24 -26 34 57.4   10 8.13     ~ 1013 0
83 ESO 474-36 G 00 52 46.1613745488 -22 58 29.748289440   15.29   13.85   ~ 19 0
84 RGO 11168 G 00 53 04.2679212206 -26 10 14.451648092   14.7 15.45 14.4 15.402 ~ 4 0
85 LEDA 786999 G 00 53 04.6 -24 42 15           ~ 4 0
86 AT 2019npz ev 00 53 05.560 -24 21 38.71           ~ 1 0
87 SN 2019npv SN* 00 53 32.316 -23 49 58.50           SNIbc 5 0
88 AT 2019qcc ev 00 53 49.820 -24 45 49.58           ~ 1 0
89 2MASX J00535773-2432353 G 00 53 57.7163640120 -24 32 35.367599040   16.89   15.73   ~ 5 0
90 AT 2019aacd ev 00 54 11.280 -24 56 17.66           ~ 2 0
91 2MASX J00543767-2504015 G 00 54 37.6911623496 -25 04 01.894389096   16.60   15.36   ~ 5 0
92 2dFGRS TGS144Z110 GiC 00 54 49.1599508472 -26 22 16.111683264   16.04 14.26 14.949   ~ 14 0
93 2dFGRS TGS144Z105 GiC 00 54 53.4 -26 22 52   17.512   16.730   ~ 5 0
94 AT 2019nuk ev 00 54 57.827 -26 08 04.61           ~ 2 0
95 LEDA 3235434 G 00 55 09.1454485344 -25 27 20.252827908   16.575   15.335   ~ 5 0
96 2MASX J00551286-2619515 GiC 00 55 12.8396605272 -26 19 50.999595492   17.15 16.38     ~ 8 0
97 2MASX J00551306-2402385 G 00 55 13.0391077056 -24 02 38.867341776   16.41       ~ 13 0
98 2dFGRS TGS144Z081 GiC 00 55 13.4868575880 -26 19 16.944315456   15.81 13.19 14.433   ~ 18 0
99 AT 2019nul SN? 00 55 16.454 -26 56 35.04           ~ 3 0
100 AT 2019num SN* 00 55 31.602 -22 58 08.48           SNII 5 0
101 AT 2019nvd ev 00 55 42.301 -24 41 49.93           ~ 1 0
102 AT 2019osy ev 00 55 47.000 -27 04 33.00           ~ 5 0
103 NAME S190814bv GWE 00 55.8 -27 05           ~ 12 0
104 AT 2019npw SN* 00 55 52.399 -25 46 59.81           SNIIb 6 0
105 AT 2019nve ev 00 56 05.510 -24 38 26.40           ~ 1 0
106 AT 2019nqw ev 00 56 46.693 -25 09 33.29           ~ 1 0
107 AT 2019nun ev 00 56 48.599 -24 54 30.48           ~ 2 0
108 AT 2019qbz ev 00 56 53.987 -27 59 21.37           ~ 2 0
109 2MASX J00570111-2350142 G 00 57 01.1094313608 -23 50 14.322016752   15.86       ~ 7 0
110 AT 2019opp ev 00 57 38.254 -25 16 45.00           ~ 2 0
111 AT 2019nys ev 00 57 56.904 -24 34 00.48           ~ 2 0
112 AT 2019nzd ev 00 58 06.456 -24 50 14.28           ~ 1 0
113 AT 2019obc SN* 00 58 16.005 -24 08 22.92           SNIa 3 0
114 AT 2019oab ev 00 58 59.398 -25 46 12.66           ~ 2 0
115 AT 2019omt ev 00 59 26.742 -25 59 41.28           ~ 3 0
116 AT 2019ntr SN* 01 00 01.843 -26 42 51.32           SNII 6 0
117 NAME Sculptor Dwarf Galaxy G 01 00 09.4 -33 42 32   9.79 8.6 8.81   ~ 1296 4
118 AT 2019oks ev 01 02 08.319 -24 54 21.70           ~ 2 0
119 AT 2019nqq SN? 01 23 49.22 -33 02 05.0           ~ 6 0
120 2MASX J01283488-3217472 G 01 28 34.8483141672 -32 17 47.127219072   16.10       ~ 5 0
121 AT 2019nqc SN* 01 29 03.671 -32 42 18.56           SNII 4 0
122 6dFGS gJ012922.3-325058 LSB 01 29 22.2796693968 -32 50 58.213352940   15.96   14.739   ~ 6 0
123 6dFGS gJ013012.0-325413 BiC 01 30 11.9752237320 -32 54 12.710689416   16.25   14.96   ~ 7 0
124 2dFGRS TGS452Z082 G 01 31 45.2747265600 -32 24 55.993721652   16.42   14.876   ~ 8 0
125 2dFGRS TGS508Z132 G 01 32 04.3742217696 -33 48 10.501990848   15.583   14.464   ~ 10 0
126 AT 2019nqs ev 01 33 35.164 -31 46 48.48           ~ 4 0
127 AT 2019omu ev 01 33 58.890 -34 20 20.01           ~ 2 0
128 AT 2019nte ev 01 34 13.766 -31 43 18.12           ~ 5 0
129 AT 2019nqr ev 01 34 17.649 -32 44 30.41           ~ 5 0
130 2dFGRS TGS452Z029 BiC 01 34 22.7796084768 -32 50 07.689294924   15.588   14.110   ~ 13 0
131 AT 2019ntn ev 01 34 53.352 -31 22 49.74           ~ 5 0
132 2dFGRS TGS509Z157 G 01 35 30.5622841440 -32 58 14.012020308   16.130   14.793   ~ 9 0
133 AT 2019omx ev 01 36 44.246 -33 18 09.64           ~ 5 0
134 6dFGS gJ013720.2-331951 G 01 37 20.1612593136 -33 19 51.064815720   15.890   14.991   ~ 6 0
135 AT 2019omv ev 01 39 54.812 -33 23 01.39           ~ 2 0
136 GRB 130603B gB 11 28 48.16 +17 04 18.2           ~ 322 0
137 Fermi bn150101641 gB 12 32 04.98 -10 56 00.7           ~ 127 1
138 NGC 4993 GiG 13 09 47.6908761600 -23 23 02.314044636   13.34   11.92   ~ 309 0
139 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 1692 0
140 GRB 070809 gB 13 35 04.2 -22 07 07           ~ 142 0
141 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 104 0
142 GRB 060614 gB 21 23 32.140 -53 01 36.10 18.89 20.12 19.54     ~ 569 1
143 GRB 050709 gB 23 01 26.960 -38 58 39.50           ~ 289 1
144 GrW 150914 GWE ~ ~           ~ 534 1

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2023.06.01-05:18:37

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