2025A&A...695A..29S


Query : 2025A&A...695A..29S

2025A&A...695A..29S - Astronomy and Astrophysics, volume 695A29 (2025/3-1)

The diversity of strongly interacting Type IIn supernovae.

SALMASO I., CAPPELLARO E., TARTAGLIA L., ANDERSON J.P., BENETTI S., BRONIKOWSKI M., CAI Y.-Z., CHARALAMPOPOULOS P., CHEN T.-W., CONCEPCION E., ELIAS-ROSA N., GALBANY L., GROMADZKI M., GUTIERREZ C.P., KANKARE E., LUNDQVIST P., MATILAINEN K., MAZZALI P.A., MORAN S., MULLER-BRAVO T.E., NICHOLL M., PASTORELLO A., PESSI P.J., PESSI T., PETRUSHEVSKA T., PIGNATA G., REGUITTI A., SOLLERMAN J., SRIVASTAV S., STRITZINGER M., TOMASELLA L. and VALERIN G.

Abstract (from CDS):

Context. At late stages, massive stars experience strong mass-loss rates, losing their external layers and thus producing a dense H-rich circumstellar medium (CSM). After the explosion of a massive star, the collision and continued interaction of the supernova (SN) ejecta with the CSM power the SN light curve through the conversion of kinetic energy into radiation. When the interaction is strong, the light curve shows a broad peak and high luminosity that lasts for several months. For these SNe, the spectral evolution is also slower compared to non-interacting SNe. Notably, energetic shocks between the ejecta and the CSM create the ideal conditions for particle acceleration and the production of high-energy (HE) neutrinos above 1 TeV.
Aims. We study four strongly interacting Type IIn SNe, 2021acya, 2021adxl, 2022qml, and 2022wed, in order to highlight their peculiar characteristics, derive the kinetic energy of their explosion and the characteristics of the CSM, infer clues on the possible progenitors and their environment, and relate them to the production of HE neutrinos.
Methods. We analysed spectro-photometric data of a sample of interacting SNe to determine their common characteristics and derive the physical properties (radii and masses) of the CSM and the ejecta kinetic energies and compare them to HE neutrino production models.
Results. The SNe analysed in this sample exploded in dwarf star-forming galaxies, and they are consistent with energetic explosions and strong interaction with the surrounding CSM. For SNe 2021acya and 2022wed, we find high CSM masses and mass-loss rates, linking them to very massive progenitors. For SN 2021adxl, the spectral analysis and less extreme CSM mass suggest a stripped-envelope massive star as a possible progenitor. SN 2022qml is marginally consistent with being a Type Ia thermonuclear explosion embedded in a dense CSM. The mass-loss rates for all the SNe are consistent with the expulsion of several solar masses of material during eruptive episodes in the last few decades before the explosion. Finally, we find that the SNe in our sample are marginally consistent with HE neutrino production.

Abstract Copyright: © The Authors 2025

Journal keyword(s): neutrinos - supernovae: general - supernovae: individual: 2021acya - supernovae: individual: 2021adxl - supernovae: individual: 2022qml - supernovae: individual: 2022wed

VizieR on-line data: <Available at CDS (J/A+A/695/A29): ph21acya.dat ph21adxl.dat ph22qml.dat ph22wed.dat ha21acya.dat ha21adxl.dat ha22qml.dat ha22wed.dat hb21acya.dat hb21adxl.dat hb22qml.dat hb22wed.dat sp21acya.dat sp21adxl.dat sp22qml.dat sp22wed.dat>

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 - 2026
#notes
1 ASASSN -14il SN* 00 45 32.55 -14 15 34.6           SNIIn 11 0
2 SN 2002ic SN* 01 30 02.55 +21 53 06.9     18.5     SNIapec 252 1
3 GALEXASC J040213.69-282329.8 UV 04 02 13.69 -28 23 29.8           ~ 1 0
4 SN 2021acya SN* 04 02 13.760 -28 23 29.72           SNIIn 2 0
5 SN 1997cy SN* 04 32 54.86 -61 42 57.5     17.4     SNIIn 146 3
6 2MASS J07241507+1904554 NIR 07 24 15.07273 +19 04 55.4915           ~ 1 0
7 SN 2022wed SN* 07 24 15.497 +19 04 52.71           SNIIn 1 0
8 WISEA J072415.72+190456.3 MIR 07 24 15.7213 +19 04 56.320           ~ 1 0
9 WISEA J072415.95+190449.4 MIR 07 24 15.9596 +19 04 49.497           ~ 1 0
10 SN 2005kj SN* 08 40 09.18 -05 36 02.2     16.3     SNIIn 26 1
11 SN 2005ip SN* 09 32 06.42 +08 26 44.4 18.1 18.7 18.5     SNIIn 230 1
12 SN 2023uqf SN* 09 33 49.151 +25 06 56.86           SNIbn 2 0
13 SN 2010jl SN* 09 42 53.33 +09 29 41.8           SNIIn 350 1
14 * 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
15 SN 1988Z SN* 10 51 50.10 +16 00 00.5   16.8       SNIIn 385 1
16 SN 2015bn SN* 11 33 41.57 +00 43 32.2           SLSN-I 157 0
17 SN 2013L SN* 11 45 29.55 -50 35 53.1           SNIIn 35 1
18 SN 1998S SN* 11 46 06.1 +47 28 55     12.2     SNIIn 517 1
19 GALEXASC J114806.87-123843.3 MIR 11 48 06.88 -12 38 41.3           ~ 3 0
20 SN 2021adxl SN* 11 48 06.940 -12 38 41.71           SLSN-II 8 0
21 SN 2006aa SN* 11 53 19.89 +20 45 18.2     18.1     SNIIn 30 1
22 SN 2022iaz SN* 12 30 31.315 -19 04 42.13           SNIIn 1 0
23 SN 2021qim SN* 12 42 45.210 +73 08 20.33           SNIIn 1 0
24 SN 2011fh SN* 12 56 14.01 -29 29 54.8           SNIIn 21 1
25 SN 2021crx SN* 13 21 53.965 +08 36 20.17           SNII 1 0
26 SN 2022owx SN* 14 24 36.230 +04 33 30.49           SNIIn 1 0
27 SN 2020faa SN* 14 47 09.469 +72 44 11.56           SNII 22 0
28 SN 2023awp SN* 15 30 01.536 +12 59 15.15           SNIIn 1 0
29 SN 2021kwj SN* 18 19 49.510 +56 10 01.20           SNIIn 1 0
30 SN 2021gci SN* 18 34 40.186 +22 53 42.02           SNIIn 1 0
31 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
32 SN 2006bo SN* 20 30 41.90 +09 11 40.8     17.6     SNIIn 24 1
33 SN 2004et SN* 20 35 25.33 +60 07 17.7   12.88       SNIIP 547 1
34 SN 2022qml SN* 22 29 45.502 +13 38 24.11           SNIIn 2 0
35 SDSS J222945.52+133823.5 G 22 29 45.52332 +13 38 23.5753           ~ 1 0
36 IceCube-231004A ev ~ ~           ~ 5 0

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