2026A&A...707A.157C


Query : 2026A&A...707A.157C

2026A&A...707A.157C - Astronomy and Astrophysics, volume 707A157 (2026/3-1)

Massive stars exploding in a He-rich circumstellar medium XII. SN 2024acyl: A fast, linearly declining Type Ibn supernova with early flash-ionisation features.

CAI Y.-Z., PASTORELLO A., MAEDA K., ZHAO J.-W., WANG Z.-Y., PENG Z.-H., REGUITTI A., TARTAGLIA L., FILIPPENKO A.V., PAN Y., VALERIN G., KUMAR B., WANG Z., FRASER M., ANDERSON J.P., BENETTI S., BOSE S., BRINK T.G., CAPPELLARO E., CHEN T.-W., CHEN X.-L., ELIAS-ROSA N., ESAMDIN A., GAL-YAM A., GONZALEZ-BANUELOS M., GROMADZKI M., GUTIERREZ C.P., INSERRA C., ISKANDAR A., KANGAS T., KANKARE E., KRAVTSOV T., KUNCARAYAKTI H., LI L.-P., LIU C.-X., LIU X.-K., LUNDQVIST P., MATILAINEN K., MATTILA S., MORAN S., MULLER-BRAVO T.E., NAGAO T., PETRUSHEVSKA T., PIGNATA G., SALMASO I., SMARTT S.J., SOLLERMAN J., SRIVASTAV S., STRITZINGER M.D., WANG L.-T., YAN S.-Y., YANG Y., YANG Y.-P., ZHENG W., ZOU X.-Z., CHEN L.-Y., DU X.-L., FANG Q.-L., FIORE A., RAGOSTA F., ZHA S., ZHANG J.-J., LIU X.-W., BAI J.-M., WANG B. and WANG X.-F.

Abstract (from CDS):

We present a photometric and spectroscopic analyses of the Type Ibn supernova (SN) 2024acyl. It rises to an absolute magnitude peak of Mo = -17.58 ± 0.15 mag in 10.6 days, and displays a rapid linear post-peak light-curve decline in all bands (e.g. γ_0 - 60_(V) = 0.097 ± 0.002 mag day–1), similar to most SNe Ibn. The optical pseudobolometric light curve peaks at (3.5 ± 0.8)×1042 erg s–1, with a total radiated energy of (5.0 ± 0.4)×1048 erg. The spectra are dominated by a blue continuum at early stages, with narrow P-Cygni He I lines and flash-ionisation emission lines of C III, N III, and He II. The P-Cygni He I features gradually evolve and become emission-dominated in late-time spectra. The Hα line is detected throughout the entire spectral evolution, which indicates that the circumstellar material (CSM) is helium-rich with some residual amount of hydrogen. Our multi-band light-curve modelling yields estimates of the ejecta mass of $ M_{\mathrm{ej}} = 0.49^{+0.11}_{-0.09} \, M_{\odot} $ with a kinetic energy of $ E_{\mathrm{k}} = 0.06^{+0.01}_{-0.01} \times 10^{51}\,\mathrm{erg} $, and a 56Ni mass of MNi = 0.018 M⊙. The inferred CSM properties are characterised by a mass of $ M_{\mathrm{CSM}} = 0.51^{+0.05}_{-0.04}\, M_{\odot} $, an inner radius of R0=$ 17.8^{+3.6}_{-3.0} $ AU, and a density of $ \rho_{\mathrm{CSM}} = (8.3_{-1.2}^{+2.7})\times10^{-12} \, \mathrm{g\,cm}^{-3} $. The multi-epoch spectra are well reproduced by the CMFGEN/ he4p0 model, corresponding to a He-ZAMS mass of 4 M⊙ (H-ZAMS mass 18.11 M⊙, pre-SN mass 3.16 M⊙). These findings are consistent with a scenario of an SN powered by ejecta-CSM interaction originating from a low-mass helium star that evolved within an interacting binary system where the CSM with some residual hydrogen may originate from the mass-transfer process. We also discuss an extreme scenario involving the possible merger of a helium white dwarf. In addition, a channel of core-collapse explosion of a late-type Wolf-Rayet (WR) star with hydrogen, or a transitional star between an Of and a WR type (e.g. an Ofpe/WN9 star) with fallback accretion cannot be entirely ruled out.

Abstract Copyright: © The Authors 2026

Journal keyword(s): circumstellar matter - supernovae: general - supernovae: individual: SN 2024acyl

VizieR on-line data: <Available at CDS (J/A+A/707/A157): table1.dat>

Simbad objects: 30

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Number of rows : 30
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 OGLE 2014-SN-131 SN* 01 14 00.81 -77 06 16.5           SNIbn 19 0
2 SN 2018gjx SN* 02 16 15.6 +28 35 29           SNIIb 25 0
3 Z 505-52 G 02 46 01.1696572584 +28 01 41.018209032   15.6       ~ 22 0
4 SN 2024acyl SN* 02 46 05.326 +28 01 17.91           ~ 1 0
5 OGLE 2012-SN-6 SN* 03 33 34.79 -74 23 40.1           SNIbn 42 0
6 SN 2019cj SN* 04 56 22.92 -46 02 11.2           ~ 5 0
7 SN 2015U SN* 07 28 53.87 +33 49 10.6           SNIbn 47 1
8 SN 2010al SN* 08 14 15.91 +18 26 18.2           SNIInpec 77 1
9 PS1-12sk SN* 08 44 54.860 +42 58 16.89           SNIbn 40 0
10 Z 208-42 rG 08 44 56.6392742400 +42 58 35.730543828   15.4 14.40     ~ 34 1
11 SN 2023utc SN* 09 11 59.155 +53 43 02.60           SNIbn 5 0
12 SN 2006jc SN* 09 17 20.78 +41 54 32.7     13.8     SNIbn 380 1
13 SN 2019wep SN* 11 04 37.033 +45 58 38.95           SNII-pec 13 0
14 SN 1998S SN* 11 46 06.1 +47 28 55     12.2     SNIIn 517 1
15 SN 2019uo SN* 12 02 36.602 +41 03 41.92           SNIbn 27 0
16 iPTF 15ul SN* 12 14 03.76 +47 54 03.9           ~ 24 0
17 SN 2005la SN* 12 52 15.68 +27 31 52.5     17.6     SNIbn/IIbn 72 1
18 ASASSN -14ms SN* 13 04 08.69 +52 18 46.5           SNIbn 19 0
19 SN 2021foa SN* 13 17 12.370 -17 15 26.02           SNIIn 21 0
20 SN 2023emq SN* 13 34 22.033 -23 43 51.45           SNIbn 6 0
21 SN 2020bqj SN* 15 33 40.48 +34 28 44.3           SNIb 10 0
22 SN 2017ckj SN* 16 09 44.400 +48 02 07.26           ~ 3 0
23 iPTF 13beo SN* 16 12 26.63 +14 19 18.0           SNIbn 30 0
24 ASASSN -15ed SN* 16 48 25.16 +50 59 30.7           SNIbn 32 0
25 SN 1999cq SN* 18 32 07.10 +37 36 44.3     15.8     SNIb/c 59 1
26 SN 2015G SN* 20 37 25.58 +66 07 11.5           SNIbn 42 1
27 SN 2019kbj SN* 22 11 21.930 +19 37 03.48           SNIbn 9 0
28 SN 2020taz SN* 22 26 06.270 +10 33 29.65           SNIbn 2 0
29 SN 2011hw SN* 22 26 14.54 +34 12 59.1           SNIIn: 61 1
30 SN 2020nxt SN* 22 37 36.235 +35 00 07.68           SNIbn 12 0

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