2025ApJ...992..100J


Query : 2025ApJ...992..100J

2025ApJ...992..100J - Astrophys. J., 992, 100 (2025/October-2)

Final Moments. III. Explosion Properties and Progenitor Constraints of CSM-interacting Type II Supernovae.

JACOBSON-GALAN W.V., DESSART L., DAVIS K.W., BOSTROEM K.A., KILPATRICK C.D., MARGUTTI R., FILIPPENKO A.V., FOLEY R.J., CHORNOCK R., TERRERAN G., HIRAMATSU D., NEWSOME M., PADILLA GONZALEZ E., PELLEGRINO C., HOWELL D.A., ANDERSON J.P., ANGUS C.R., AUCHETTL K., BRINK T.G., CARTIER R., COULTER D.A., DE BOER T., DROUT M.R., EARL N., ERTINI K., FARAH J.R., FARIAS D., GALL C., GAO H., GERLACH M.A., GUO F., HAYNIE A., HOSSEINZADEH G., IBIK A.L., JHA S.W., JONES D.O., LANGEROODI D., LEBARON N., MAGNIER E.A., PIRO A.L., RAIMUNDO S.I., REST A., REST S., RICH R.M., ROJAS-BRAVO C., SEARS H., TAGGART K., VILLAR V.A., WAINSCOAT R.J., WANG X.-F., WASSERMAN A.R., YAN S., YANG Y., ZHANG J. and ZHENG W.

Abstract (from CDS):

We present analysis of the plateau and late-time phase properties of a sample of 39 Type II supernovae (SNe II) that show narrow, transient, high-ionization emission lines (i.e., “IIn-like”) in their early-time spectra from interaction with confined, dense circumstellar material (CSM). Originally presented by W. V. Jacobson-Galán et al., this sample also includes multicolor light curves and spectra extending to late-time phases of 35 SNe with no evidence for IIn-like features at <2 days after first light. We measure photospheric phase light-curve properties for the distance-corrected sample and find that SNe II with IIn-like features have significantly higher luminosities and decline rates at +50 days than the comparison sample, which could be connected to inflated progenitor radii, lower ejecta mass, and/or persistent CSM interaction. However, we find no statistical evidence that the measured plateau durations and 56Ni masses of SNe II with and without IIn-like features arise from different distributions. We estimate progenitor zero-age main-sequence (ZAMS) masses for all SNe with nebular spectroscopy through spectral model comparisons and find that most objects, both with and without IIn-like features, are consistent with progenitor masses ≤12.5 M⊙. Combining progenitor ZAMS masses with CSM densities inferred from early-time spectra suggests multiple channels for enhanced mass loss in the final years before core collapse, such as a convection-driven chromosphere or binary interaction. Finally, we find spectroscopic evidence for ongoing ejecta-CSM interaction at radii >1016 cm, consistent with substantial progenitor mass-loss rates of ∼10–4-10–5M⊙ yr–1 (vw < 50 km s–1) in the final centuries to millennia before explosion.

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

Journal keyword(s): Type II supernovae - Core-collapse supernovae - Supernovae - Red supergiant stars

Simbad objects: 76

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Number of rows : 76
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 2018fif SN* 00 09 26.555 +47 21 14.73           SNII 15 0
2 iPTF 13iqb SN* 00 34 04.84 -09 42 17.9           SNIIn 88 0
3 AT 2022ibv SN* 00 49 04.170 -29 22 29.69           SNII 3 0
4 SN 2019ust SN* 00 54 22.41502 +31 40 12.6548           ~ 7 0
5 SN 2020abjq SN* 01 06 14.630 +03 34 26.08           SNII 3 0
6 SN 2021ass SN* 01 50 10.130 +27 38 42.79           SNII 3 0
7 SN 2021afkk SN* 02 29 59.968 +28 38 03.07           SNII 5 0
8 SN 2017gmr SN* 02 35 30.15 -09 21 15.0           SNII 64 0
9 SN 2021aaqn SN* 02 37 58.184 -01 49 53.21           SNII 4 0
10 SN 2021yja SN* 03 24 21.180 -21 33 56.20           SNIIP 39 0
11 SN 2018kpo SN* 03 40 43.05 -06 25 24.1           SNII 9 0
12 CRTS CSS101208 J051640+064754 SN* 05 16 40.52 +06 47 53.8           SNII 12 0
13 SN 1987A SN* 05 35 27.98840 -69 16 11.1134           SNIIpec 5203 2
14 SN 2021vaz SN* 05 42 01.720 +69 22 36.73           SNII 2 0
15 ASASSN -16cc SN* 05 46 23.907 -52 05 18.86           SNII 24 0
16 SN 2018lab SN* 06 16 26.520 -21 22 32.38           SNII 19 0
17 SN 2018zd SN* 06 18 03.180 +78 22 00.90           SNII 74 0
18 SN 2020abtf SN* 07 59 34.479 +15 18 00.07           SNII 2 0
19 SN 2020acbm SN* 08 04 20.304 +56 18 07.50           SNII 3 0
20 SN 2021dbg SN* 09 24 26.790 -06 34 53.15           SNII 7 0
21 SN 2019enr SN* 09 34 47.71 +10 17 12.8           SNII 4 0
22 SN 2021jtt SN* 09 41 16.452 +35 53 02.60           SNII 3 0
23 SN 2022jox SN* 09 57 44.520 -28 30 57.06           SNII 11 0
24 SN 2022ffg SN* 10 13 48.230 +18 07 38.35           SNII 4 0
25 SN 2017ahn SN* 10 37 17.450 -41 37 05.27           SNII 54 0
26 SN 2021gmj SN* 10 38 47.270 +53 30 30.31           SNII 17 0
27 SN 2014G SN* 10 54 34.13 +54 17 56.9           SNIIL 95 1
28 SN 2021zj SN* 11 16 32.710 +29 05 46.14           SNII 4 0
29 SN 2013am SN* 11 18 56.95 +13 03 49.4           SNII 52 1
30 SN 2022inn SN* 11 21 27.070 +63 01 24.60           SNII 2 0
31 SN 2021adly SN* 11 28 41.810 +35 06 45.50           ~ 3 0
32 SN 2021mqh SN* 11 39 50.482 -07 36 26.76           SNII 3 0
33 SN 2021aek SN* 11 59 48.020 -21 23 13.09           SNII 2 0
34 SN 2022jzc SN* 12 05 28.670 +50 31 36.80           SNII 2 0
35 SN 2019edo SN* 12 11 51.566 +24 08 11.67           SNII 5 0
36 SN 2020jfo SN* 12 21 50.480 +04 28 54.05           SNII 48 0
37 PTF 10gva SN* 12 23 55.40 +10 34 50.7       18.2   SNII 15 1
38 SN 2022fuc SN* 12 34 34.230 +63 31 06.46           SNIIP 2 0
39 SN 2020fqv SN* 12 36 33.260 +11 13 53.87           SNII 20 0
40 SN 2016X SN* 12 55 15.50 +00 05 59.7           SNIIb 61 0
41 SN 2021can SN* 12 55 30.795 +30 01 40.80           SNII 3 0
42 SN 2020nif SN* 13 04 13.740 -10 21 03.49           SNII 5 0
43 SN 2022frq SN* 13 27 56.880 -13 24 59.33           SNII 2 0
44 SN 2021gvm SN* 13 30 01.224 +13 24 40.28           SNII 2 0
45 SN 2021apg SN* 13 41 19.244 +24 29 43.95           SNII 5 0
46 SN 2021rhk SN* 14 03 02.405 +08 45 56.46           SNII 3 0
47 SN 2023ixf SN* 14 03 38.562 +54 18 41.94           SNII 209 0
48 SN 2020mjm SN* 14 29 29.330 -00 01 17.76           SNII 3 0
49 SN 2013ab SN* 14 32 44.49 +09 53 12.3           SNIIP 71 1
50 SN 2020tlf SN* 14 40 10.030 +42 46 39.64           SNII(n) 55 0
51 SN 2020pni SN* 15 03 49.960 +42 06 50.51           SNII 34 0
52 SN 2021wvd SN* 15 10 34.983 +13 27 30.73           SNII 2 0
53 SN 2022pgf SN* 15 11 41.900 +59 49 12.29           SNIIp 3 0
54 AT 2022prv SN? 15 40 07.750 +20 40 31.78           SNII 6 0
55 ASASSN -16eh SN* 15 40 29.233 +00 54 36.38           SNIbn 12 0
56 SN 2020sic SN* 15 47 45.110 +28 38 25.22           SNII 2 0
57 SN 2022dml SN* 16 17 29.130 +14 25 04.53           SNII 4 0
58 SN 2021ont SN* 16 26 42.476 +39 08 42.98           SNII 2 0
59 SN 2020lfn SN* 16 26 56.890 +20 14 45.20           SN.II 5 0
60 SN 2020ekk SN* 16 44 45.150 +22 30 47.74           SNII 4 0
61 SN 2018dfc SN* 16 48 07.760 +24 18 14.87           SNII 8 0
62 SN 2019nvm SN* 17 25 38.667 +59 26 48.26           SN.II 11 0
63 SN 2019pjs SN* 18 04 40.340 +21 38 04.24           SNII 5 0
64 SN 2019qch SN* 18 29 13.80960 +41 02 32.4337           ~ 6 0
65 SN 2017eaw SN* 20 34 44.238 +60 11 36.00           SNIIP 180 0
66 SN 2020dpw SN* 20 37 10.550 +66 06 10.66           SNIIP 8 0
67 SN 2018cuf SN* 21 16 11.580 -64 28 57.26           SNII 17 0
68 SN 2022ovb SN* 22 22 29.550 +36 00 17.86           SNII 2 0
69 SN 2021ucg SN* 22 47 37.677 +39 52 59.52           SNII 2 0
70 SN 2020xua SN* 22 51 22.180 +32 21 04.72           SNII 5 0
71 SN 2021uoy SN* 22 55 37.453 +19 10 25.79           SNII 4 0
72 SN 2021tyw SN* 23 05 56.460 +14 21 27.72           SNII 3 0
73 SN 2013fs SN* 23 19 44.70 +10 11 05.0           SNIIP 159 1
74 SN 2015bf SN* 23 24 49.03 +15 16 52.0           SNII 19 1
75 SN 2021qvr SN* 23 28 26.650 +22 25 11.89           SNII 4 0
76 SN 2013ft SN* 23 41 35.20 +03 43 30.5           SNIIP 11 1

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