2025ApJ...989..182G


Query : 2025ApJ...989..182G

2025ApJ...989..182G - Astrophys. J., 989, 182 (2025/August-3)

Evidence for an Instability-induced Binary Merger in the Double-peaked, Helium-rich Type IIn Supernova 2023zkd.

GAGLIANO A., VILLAR V.A., MATSUMOTO T., JONES D.O., RANSOME C.L., NUGENT A.E., HIRAMATSU D., AUCHETTL K., TSUNA D., DONG Y., GOMEZ S., ALEO P.D., ANGUS C.R., DE BOER T., BOSTROEM K.A., CHAMBERS K.C., COULTER D.A., DAVIS K.W., FAIRLAMB J.R., FARAH J., FARIAS D., FOLEY R.J., GALL C., GAO H., GONZALEZ E.P., HOWELL D.A., HUBER M.E., KILPATRICK C.D., LIN C.-C., LOWE T.B., MacLEOD M.E., MAGNIER E.A., McCULLY C., MINGUEZ P., NARAYAN G., NEWSOME M., PATRA K.C., REST A., REST S., SMARTT S., SMITH K.W., TERRERAN G., WAINSCOAT R.J., WANG Q., YADAVALLI S.K. and ZENATI Y.

Abstract (from CDS):

We present ultraviolet to infrared observations of the extraordinary Type IIn supernova 2023zkd (SN 2023zkd). Photometrically, it exhibits persistent and luminous precursor emission spanning ∼4 yr preceding discovery (Mr ≈ -15 mag, 1500 days in the observer frame), followed by a secondary stage of gradual brightening in its final year. Post-discovery, it exhibits two photometric peaks of comparable brightness (Mr ≲ -18.7 mag and Mr ≈ -18.4 mag, respectively) separated by 240 days. Spectroscopically, SN 2023zkd exhibits highly asymmetric and multicomponent Balmer and He I profiles that we attribute to ejecta interaction with fast-moving (1000-2000 km s–1) He-rich polar material and slow-moving (∼400 km s–1) equatorially distributed H-rich material. He II features also appear during the second light curve peak and evolve rapidly. Shock-driven models fit to the multiband photometry suggest that the event is powered by interaction with ∼5-6 M⊙ of CSM, with 2-3 M⊙ associated with each light curve peak, expelled during mass-loss episodes ∼3-4 yr and ∼1-2 yr prior to explosion. The observed precursor emission, combined with the extreme mass-loss rates required to power each light curve peak, favors either super-Eddington accretion onto a black hole or multiple long-lived eruptions from a massive star to luminosities that have not been previously observed. We consider multiple progenitor scenarios for SN 2023zkd, and find that the brightening optical precursor and inferred explosion properties are most consistent with a massive (MZAMS ≥ 30 M⊙) and partially stripped He star undergoing an instability-induced merger with a black hole companion.

Abstract Copyright: © 2025. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Core-collapse supernovae - Circumstellar matter - Spectroscopy - Photometry

Status at CDS : Large table(s) will be appraised for possible ingestion in VizieR.

Simbad objects: 44

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Number of rows : 44
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 SN 2022jli SN* 00 34 45.690 -08 23 12.16           SNIc 24 0
2 SN 2005gl SN* 00 49 50.02 +32 16 56.8       17.0   SNIIn 162 2
3 HD 5980 WR* 00 59 26.5838833944 -72 09 53.927337312   11.13 11.31   11.029 WN4+O7I: 419 1
4 SWIFT J0243.6+6124 HXB 02 43 40.4252869512 +61 26 03.757456824   13.71 12.84 12.57   O9.5Ve 208 0
5 PTF 10dk SN* 05 08 21.54 +00 12 42.9           SNII 8 0
6 V* S Dor sg* 05 18 14.3570612088 -69 15 01.149576912 9.08 10.39 10.25 9.74 9.14 Be3 395 0
7 SN 2019stc SN* 06 54 23.103 +17 29 31.35           SNIc 28 0
8 SN 2016jbu SN* 07 36 25.98 -69 32 55.4           SNII 45 0
9 SN 2019cad SN* 09 08 42.971 +44 48 46.04           SNIc 19 0
10 SN 2015bh SN* 09 09 34.96 +33 07 20.4           SNIIn 83 1
11 SN 2006jc SN* 09 17 20.78 +41 54 32.7     13.8     SNIbn 380 1
12 SN 2020jhs SN* 09 28 14.09932 +25 40 13.3831           ~ 3 0
13 SN 2010jl SN* 09 42 53.33 +09 29 41.8           SNIIn 350 1
14 SN 2020acct SN* 09 44 56.060 +31 05 45.77           SNIIn 6 0
15 SN 2005bf SN* 10 23 56.99 -03 11 29.3     18.0     SNIb 225 1
16 NAME Homunculus Nebula ISM 10 45 03.5 -59 41 04           ~ 379 1
17 * eta Car s*b 10 45 03.545808 -59 41 03.95124 6.37 7.03 6.48 6.123 4.41 LBV 2543 0
18 CRTS CSS140222 J112037+302809 SN* 11 20 37.10 +30 28 08.9           ~ 4 0
19 SN 2022xxf SN* 11 30 05.940 +09 16 57.37           SNIc-BL 23 0
20 SN 2013L SN* 11 45 29.55 -50 35 53.1           SNIIn 35 1
21 SN 2021adxl SN* 11 48 06.940 -12 38 41.71           SLSN-II 8 0
22 SN 2016iet SN* 12 32 33.230 +27 07 15.49           SNI 20 0
23 PTF 09uy SN* 12 43 55.771 +74 41 07.58           ~ 5 0
24 SN 2005la SN* 12 52 15.68 +27 31 52.5     17.6     SNIbn/IIbn 72 1
25 SN 2016bdu SN* 13 10 13.950 +32 31 14.07           SNIIn 35 0
26 SN 2021foa SN* 13 17 12.370 -17 15 26.02           SNIIn 21 0
27 MCG-03-34-063 Sy2 13 22 19.0228826784 -16 42 30.084610752   14   13.77   ~ 60 3
28 ASASSN -15ua SN* 13 34 54.473 +10 59 04.69           SNIIn 10 0
29 [JRW2005b] 122 UX? 14 03 32.38 +54 21 03.0   21.13       ~ 120 0
30 SN 2023ixf SN* 14 03 38.562 +54 18 41.94           SNII 209 0
31 SN 2020tlf SN* 14 40 10.030 +42 46 39.64           SNII(n) 55 0
32 iPTF 15akq SN* 15 03 51.29 +33 33 18.1           ~ 14 0
33 SN 2023zkd SN* 15 48 47.546 +09 12 00.14           SNIbn 2 0
34 PTF 10uiz SN* 17 14 30.8369 +21 25 59.709           ~ 3 0
35 SN 2010mc SN* 17 21 30.68 +48 07 47.4           SNIIn 101 1
36 SN 2023aew SN* 17 40 51.370 +66 12 22.75           SNIIb 7 0
37 PTF 09bcl SN* 18 06 26.78 +17 51 43.0           SNII 6 0
38 * P Cyg s*b 20 17 47.2019733389 +38 01 58.549132671 4.66 5.24 4.82 4.28 4.02 B1-2Ia-0ep 1200 1
39 SN 2010bt SN* 21 48 20.22 -34 57 16.5           SNIIn 20 1
40 SN 2009ip s*b 22 23 08.26 -28 56 52.4           LBV 406 0
41 SN 2021qqp SN* 22 32 40.416 +25 34 34.75           SNIIn 9 0
42 SN 2014C SN* 22 37 05.60 +34 24 31.9           SNIb 167 1
43 HD 215227 HXB 22 42 57.3031579265 +44 43 18.259103226 8.07 8.84 8.78     B1.5-2III 157 0
44 SN 1996al SN* 23 33 16.1 -54 05 02     14.0     SNII 43 1

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