2023ApJ...943...42C


Query : 2023ApJ...943...42C

2023ApJ...943...42C - Astrophys. J., 943, 42 (2023/January-3)

The Hydrogen-poor Superluminous Supernovae from the Zwicky Transient Facility Phase I Survey. II. Light-curve Modeling and Characterization of Undulations.

CHEN Z.H., YAN L., KANGAS T., LUNNAN R., SOLLERMAN J., SCHULZE S., PERLEY D.A., CHEN T.-W., TAGGART K., HINDS K.R., GAL-YAM A., WANG X.F., DE K., BELLM E., BLOOM J.S., DEKANY R., GRAHAM M., KASLIWAL M., KULKARNI S., LAHER R., NEILL D. and RUSHOLME B.

Abstract (from CDS):

We present analysis of the light curves (LCs) of 77 hydrogen-poor superluminous supernovae (SLSNe I) discovered during the Zwicky Transient Facility Phase I operation. We find that the majority (67%) of the sample can be fit equally well by both magnetar and ejecta-circumstellar medium (CSM) interaction plus 56Ni decay models. This implies that LCs alone cannot unambiguously constrain the physical power sources for an SLSN I. However, 23% of the sample show inverted V-shape, steep-declining LCs or features of long rise and fast post-peak decay, which are better described by the CSM+Ni model. The remaining 10% of the sample favors the magnetar model. Moreover, our analysis shows that the LC undulations are quite common, with a fraction of 18%-44% in our gold sample. Among those strongly undulating events, about 62% of them are found to be CSM-favored, implying that the undulations tend to occur in the CSM-favored events. Undulations show a wide range in energy and duration, with median values (and 1σ errors) being as $1.7{ \% }_{-0.7 \% }^{+1.5 \% }\,{E}_{\mathrm{rad},\mathrm{total}}$ and ${28.8}_{-9.1}^{+14.4}$ days, respectively. Our analysis of the undulation timescales suggests that intrinsic temporal variations of the central engine can explain half of the undulating events, while CSM interaction (CSI) can account for the majority of the sample. Finally, all of the well-observed He-rich SLSNe Ib either have strongly undulating LCs or the LCs are much better fit by the CSM+Ni model. These observations imply that their progenitor stars have not had enough time to lose all of the He-envelopes before supernova explosions, and H-poor CSM are likely to present in these events.

Abstract Copyright: © 2023. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Supernovae

VizieR on-line data: <Available at CDS (J/ApJ/943/42): tablea1.dat tablea2.dat>

Simbad objects: 88

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Number of rows : 88
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 2019lsq SN* 00 04 40.600 +42 52 11.35           SLSN-I 12 0
2 SN 2019szu SN* 00 10 13.140 -19 41 32.46           SLSN-I 14 0
3 SN 2020afag SN* 00 15 46.250 +47 00 08.50           ~ 4 0
4 SN 2020xgd SN* 00 19 45.830 +05 08 18.60           SLSN-I 7 0
5 SN 2020rmv SN* 00 40 00.187 -14 35 25.14           SLSN-I 11 0
6 SN 2019nhs SN* 00 52 01.453 +07 36 59.80           SLSN-I 10 0
7 SN 2019sgg SN* 01 01 11.77 +14 01 35.4           SLSN-I 6 0
8 SN 2019sgh SN* 01 12 39.420 +36 28 24.80           SLSN-I 9 0
9 DES14X3taz SN* 02 28 04.46 -04 05 12.7           SLSN-I 47 0
10 SN 2019otl SN* 02 52 21.629 -17 48 12.50           SLSN-I 7 0
11 SN 2019aamu SN* 02 55 08.890 +11 27 22.40           ~ 5 0
12 SN 2018hti SN* 03 40 53.754 +11 46 37.29           SLSN-I 30 0
13 SN 2018ibb SN* 04 38 56.95 -20 39 44.0           SLSN-I 31 0
14 SN 2019stc SN* 06 54 23.103 +17 29 31.35           SNIc 28 0
15 SN 2018lzw SN* 07 39 32.760 +27 44 02.70           SLSN-I 5 0
16 SN 2018gkz SN* 07 58 11.548 +19 31 07.95           SLSN-I 11 0
17 SN 2020dlb SN* 08 08 34.142 +34 44 13.12           ~ 4 0
18 SN 2020ank SN* 08 16 14.653 +04 19 26.88           ~ 15 0
19 SN 2019cdt SN* 08 17 53.930 +65 28 46.52           SLSN-I 9 0
20 SN 2019xdy SN* 08 24 51.320 +22 10 46.02           ~ 4 0
21 SN 2019ujb SN* 09 03 15.170 +40 14 32.50           SLSN-I 12 0
22 SN 2019vvc SN* 09 13 30.130 +44 46 26.22           ~ 4 0
23 SN 2020iyj SN* 09 15 36.647 +53 27 32.03           ~ 4 0
24 SN 2018lfe SN* 09 33 29.556 +00 03 08.39           SLSN-I 11 0
25 SN 2019dgr SN* 09 45 32.682 +04 56 02.21           ~ 5 0
26 SN 2019unb SN* 09 47 57.02 +00 49 36.0           SLSN-I 16 0
27 SN 2019bgu SN* 09 57 15.343 +32 00 05.62           SLSN-I 6 0
28 LSQ 14bdq SN* 10 01 41.60 -12 22 13.4           SLSN-I 70 0
29 SN 2019J SN* 10 03 46.771 +06 46 24.44           SLSN-I 7 0
30 SN 2019zbv SN* 10 15 01.124 +43 24 53.68           SLSN-I 10 0
31 SN 2017egm SN* 10 19 05.620 +46 27 14.08           SLSN-I 93 0
32 SN 2019gam SN* 10 19 18.32 +17 12 42.6           SLSN-I 7 0
33 SN 2020afah SN* 10 20 18.320 +53 19 21.40           ~ 5 0
34 SN 2018bgv SN* 11 02 30.290 +55 35 55.79           SLSN-I 18 0
35 SN 2020kox SN* 11 06 04.908 +26 17 27.97           ~ 4 0
36 SN 2019dlr SN* 11 17 34.180 +00 30 02.79           SLSN-I 7 0
37 SN 2015bn SN* 11 33 41.57 +00 43 32.2           SLSN-I 157 0
38 SN 2019cca SN* 12 02 51.400 -16 39 47.66           SLSN-I 9 0
39 SN 2018kyt SN* 12 27 56.23 +56 23 35.6           SLSN-I 14 0
40 SN 2018lzv SN* 12 44 02.320 +56 01 44.50           SLSN-I 5 0
41 SN 2019aamv SN* 12 45 01.650 +33 33 14.10           ~ 3 0
42 SN 2020aup SN* 13 09 44.453 +12 29 13.69           ~ 4 0
43 SN 2018avk SN* 13 11 27.750 +65 38 17.16           SLSN-I 14 0
44 SN 2011ke SN* 13 50 57.77 +26 16 42.8     18.6     SLSN-I 92 1
45 SN 2018don SN* 13 55 08.64 +58 29 41.9           SLSN-I 22 0
46 SN 2019kwu SN* 13 57 39.770 +64 21 18.60           SLSN-I 6 0
47 SN 2019fiy SN* 14 05 46.728 +33 27 38.19           SLSN-I 7 0
48 SN 2019kcy SN* 14 08 19.781 +08 58 01.01           SLSN-I 9 0
49 SN 2020fvm SN* 14 12 45.972 +34 44 16.24           ~ 5 0
50 SN 2019kws SN* 14 15 04.460 +50 39 06.80           SLSN-I 8 0
51 SN 2019gqi SN* 14 21 12.014 +28 54 05.88           SLSN-I 7 0
52 SN 2020onb SN* 14 23 00.600 +49 10 40.69           SLSN-I 7 0
53 PTF 12dam SN* 14 24 46.20 +46 13 48.3           SLSN-I 172 0
54 SN 2019aamp SN* 14 37 49.270 +20 18 16.60           SLSN-I 5 0
55 SN 2020exj SN* 14 42 40.012 +30 14 39.20           SLSN-I 9 0
56 SN 2020fyq SN* 14 46 10.445 +23 48 02.03           ~ 4 0
57 SN 2019cwu SN* 14 51 37.295 +48 59 13.73           SLSN-I 8 0
58 SN 2019aamr SN* 15 29 23.550 +38 06 12.60           ~ 4 0
59 SN 2020jii SN* 15 34 55.291 +02 51 11.66           SLSN-I 5 0
60 SN 2019gfm SN* 15 35 46.593 +24 03 44.93           SLSN-I 11 0
61 SN 2018gbw SN* 15 55 38.019 +28 21 38.00           ~ 3 0
62 SN 2019aamx SN* 15 57 48.270 +27 28 03.50           ~ 3 0
63 SN 2018bsz SN* 16 09 39.110 -32 03 45.63           SNII 51 0
64 SN 2020auv SN* 16 34 12.532 +37 05 51.78           SLSN-I 8 0
65 SN 2019kwq SN* 17 07 58.840 +58 42 03.90           SLSN-I 7 0
66 SN 2020htd SN* 17 44 17.271 +38 55 30.76           ~ 5 0
67 SN 2019neq SN* 17 54 26.736 +47 15 40.56           SLSN-I 20 0
68 SN 2019eot SN* 18 00 29.941 +50 17 43.30           SLSN-I 9 0
69 SN 2018hpq SN* 18 28 41.27 +75 48 47.4           SNIc 8 0
70 SN 2018bym SN* 18 43 13.429 +45 12 28.21           SLSN-I 18 0
71 SN 2019hno SN* 19 39 12.963 +62 43 40.87           SLSN-I 7 0
72 SN 2019kwt SN* 19 39 22.590 +78 45 43.60           SLSN-I 8 0
73 SN 2019aamq SN* 20 55 36.140 -08 40 31.40           ~ 4 0
74 SN 2018fcg SN* 21 09 36.78 +33 28 59.6           SLSN-I 16 0
75 SN 2019aamt SN* 21 15 08.000 +32 43 01.30           ~ 4 0
76 ASASSN -15lh ev 22 02 15.4 -61 39 34           ~ 187 1
77 SN 2006oz SN* 22 08 53.56 +00 53 50.4           SLSN-I 90 1
78 SN 2019hge SN* 22 24 21.20 +24 47 17.1           SLSN-I 17 0
79 SN 2018lzx SN* 22 29 27.240 +13 10 39.80           ~ 4 0
80 SN 2019qgk SN* 22 29 57.566 -04 06 02.42           ~ 4 0
81 SN 2019obk SN* 22 33 54.08 -02 09 42.3           SLSN-I 8 0
82 SN 2020xkv SN* 22 37 46.345 +23 31 37.23           ~ 4 0
83 SN 2020qef SN* 22 56 10.530 +28 45 53.23           SLSN-Ib 8 0
84 SN 2001ig SN* 22 57 30.69 -41 02 25.9     14.5     SNIIb 190 1
85 SN 2018lfd SN* 23 14 59.320 +48 45 27.79           SLSN-I 7 0
86 SN 2019aams SN* 23 43 36.160 +12 29 01.00           ~ 4 0
87 SN 2019aamw SN* 23 48 54.540 +24 59 59.80           ~ 4 0
88 SN 2018gft SN* 23 57 17.941 -15 37 53.32           SLSN-I 11 0

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