2020ApJ...890..131A


Query : 2020ApJ...890..131A

2020ApJ...890..131A - Astrophys. J., 890, 131-131 (2020/February-3)

GROWTH on S190814bv: deep synoptic limits on the optical/near-infrared counterpart to a neutron star-black hole merger.

ANDREONI I., GOLDSTEIN D.A., KASLIWAL M.M., NUGENT P.E., ZHOU R., NEWMAN J.A., BULLA M., FOUCART F., HOTOKEZAKA K., NAKAR E., NISSANKE S., RAAIJMAKERS G., BLOOM J.S., DE K., JENCSON J.E., WARD C., AHUMADA T., ANAND S., BUCKLEY D.A.H., CABALLERO-GARCIA M.D., CASTRO-TIRADO A.J., COPPERWHEAT C.M., COUGHLIN M.W., CENKO S.B., GROMADZKI M., HU Y., KARAMBELKAR V.R., PERLEY D.A., SHARMA Y., VALEEV A.F., COOK D.O., FREMLING U.C., KUMAR H., TAGGART K., BAGDASARYAN A., COOKE J., DAHIWALE A., DHAWAN S., DOBIE D., GATKINE P., GOLKHOU V.Z., GOOBAR A., CHAVES A.G., HANKINS M., KAPLAN D.L., KONG A.K.H., KOOL E.C., MOHITE S., SOLLERMAN J., TZANIDAKIS A., WEBB S. and ZHANG K.

Abstract (from CDS):

On 2019 August 14, the Advanced LIGO and Virgo interferometers detected the high-significance gravitational wave (GW) signal S190814bv. The GW data indicated that the event resulted from a neutron star-black hole (NSBH) merger, or potentially a low-mass binary BH merger. Due to the low false-alarm rate and the precise localization (23 deg2 at 90%), S190814bv presented the community with the best opportunity yet to directly observe an optical/near-infrared counterpart to an NSBH merger. To search for potential counterparts, the GROWTH Collaboration performed real-time image subtraction on six nights of public Dark Energy Camera images acquired in the 3 weeks following the merger, covering >98% of the localization probability. Using a worldwide network of follow-up facilities, we systematically undertook spectroscopy and imaging of optical counterpart candidates. Combining these data with a photometric redshift catalog, we ruled out each candidate as the counterpart to S190814bv and placed deep, uniform limits on the optical emission associated with S190814bv. For the nearest consistent GW distance, radiative transfer simulations of NSBH mergers constrain the ejecta mass of S190814bv to be Mej < 0.04 M at polar viewing angles, or Mej < 0.03 M if the opacity is κ < 2 cm2g–1. Assuming a tidal deformability for the NS at the high end of the range compatible with GW170817 results, our limits would constrain the BH spin component aligned with the orbital momentum to be χ < 0.7 for mass ratios Q < 6, with weaker constraints for more compact NSs.

Abstract Copyright: © 2020. The American Astronomical Society. All rights reserved.

Journal keyword(s): Neutron stars - Binary stars - Gravitational wave sources - Gravitational waves - Transient sources - Black hole physics - Observational astronomy

VizieR on-line data: <Available at CDS (J/ApJ/890/131): table2.dat table3.dat fig3.dat fig3b.dat refs.dat>

Status at CDS : Examining the need for a new acronym.

Simbad objects: 36

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Number of rows : 36
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 AT 2019mbq SN* 00 43 20.493 -25 53 02.07           SNII 4 0
2 AT 2019odc ev 00 46 01.689 -25 27 32.94           ~ 4 0
3 AT 2019nxe SN* 00 46 16.814 -24 22 21.19           SNIa 5 0
4 AT 2019nbp SN? 00 46 57.386 -24 21 42.30           ~ 3 0
5 AT 2019tih SN? 00 47 26.661 -27 36 03.01           ~ 2 0
6 AT 2019thm SN? 00 47 56.625 -26 54 02.80           ~ 3 0
7 AT 2019nyy SN? 00 48 16.650 -26 38 26.92           ~ 3 0
8 AT 2019paw SN? 00 48 34.285 -25 05 25.90           ~ 3 0
9 AT 2019tix SN? 00 48 45.678 -24 38 50.59           ~ 3 0
10 AT 2019noq SN* 00 48 47.882 -25 18 23.46           SNII 5 0
11 AT 2019tij SN? 00 48 55.703 -22 23 36.51           ~ 1 0
12 AT 2019nuj SN? 00 49 01.738 -23 14 04.93           ~ 4 0
13 AT 2019tii SN? 00 49 35.213 -27 02 09.33           ~ 3 0
14 AT 2019ntp SN* 00 50 12.072 -26 11 52.56           SNIa 5 0
15 AT 2019nme ev 00 50 32.558 -22 13 33.70           ~ 4 0
16 AT 2019nmd ev 00 51 29.004 -22 28 16.96           ~ 4 0
17 SN 2019npv SN* 00 53 32.316 -23 49 58.50           SNIbc 6 0
18 AT 2019paa SN? 00 55 13.779 -24 07 08.46           ~ 2 0
19 AT 2019nul SN? 00 55 16.454 -26 56 35.04           ~ 4 0
20 AT 2019num SN* 00 55 31.602 -22 58 08.48           SNII 5 0
21 AT 2019npw SN* 00 55 52.399 -25 46 59.81           SNIIb 6 0
22 AT 2019tig SN? 00 58 04.300 -26 04 58.85           ~ 2 0
23 AT 2019obc SN* 00 58 16.005 -24 08 22.92           SNIa 4 0
24 AT 2019omt ev 00 59 26.742 -25 59 41.28           ~ 4 0
25 AT 2019ntr SN* 01 00 01.843 -26 42 51.32           SNII 6 0
26 AT 2019tiw SN? 01 00 05.498 -24 57 02.01           ~ 1 0
27 AT 2019nqq SN* 01 23 49.22 -33 02 05.0           SNII 6 0
28 AT 2019nqc SN* 01 29 03.671 -32 42 18.56           SNII 5 0
29 HD 9485 * 01 32 48.8060148648 -16 23 17.573818596   9.19 9.11     A0V 16 0
30 AT 2019nqs ev 01 33 35.164 -31 46 48.48           ~ 5 0
31 AT 2019nte ev 01 34 13.766 -31 43 18.12           ~ 5 0
32 AT 2019nqr SN* 01 34 17.649 -32 44 30.41           SNII 6 0
33 AT 2019ntn SN* 01 34 53.352 -31 22 49.74           SNIa-CSM 5 0
34 AT 2019omx ev 01 36 44.246 -33 18 09.64           ~ 5 0
35 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2001 0
36 SN 2005cs SN* 13 29 53.37 +47 10 28.2   14.5       SNIIP 408 1

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