2024A&A...685A..20G


Query : 2024A&A...685A..20G

2024A&A...685A..20G - Astronomy and Astrophysics, volume 685A20 (2024/5-1)

SN 2020zbf: A fast-rising hydrogen-poor superluminous supernova with strong carbon lines.

GKINI A., LUNNAN R., SCHULZE S., DESSART L., BRENNAN S.J., SOLLERMAN J., PESSI P.J., NICHOLL M., YAN L., OMAND C.M.B., KANGAS T., MOORE T., ANDERSON J.P., CHEN T.-W., GONZALEZ E.P., GROMADZKI M., GUTIERREZ C.P., HIRAMATSU D., HOWELL D.A., IHANEC N., INSERRA C., McCULLY C., MULLER-BRAVO T.E., PELLEGRINO C., PIGNATA G., PURSIAINEN M. and YOUNG D.R.

Abstract (from CDS):

SN 2020zbf is a hydrogen-poor superluminous supernova (SLSN) at z = 0.1947 that shows conspicuous C II features at early times, in contrast to the majority of H-poor SLSNe. Its peak magnitude is Mg = -21.2 mag and its rise time (≲26.4 days from first light) places SN 2020zbf among the fastest rising type I SLSNe. We used spectra taken from ultraviolet (UV) to near-infrared wavelengths to identify spectral features. We paid particular attention to the C II lines as they present distinctive characteristics when compared to other events. We also analyzed UV and optical photometric data and modeled the light curves considering three different powering mechanisms: radioactive decay of 56Ni, magnetar spin-down, and circumstellar medium (CSM) interaction. The spectra of SN 2020zbf match the model spectra of a C-rich low-mass magnetar-powered supernova model well. This is consistent with our light curve modeling, which supports a magnetar-powered event with an ejecta mass Mej = 1.5 M⊙. However, we cannot discard the CSM-interaction model as it may also reproduce the observed features. The interaction with H-poor, carbon-oxygen CSM near peak light could explain the presence of C II emission lines. A short plateau in the light curve around 35-45 days after peak, in combination with the presence of an emission line at 6580 Å, can also be interpreted as being due to a late interaction with an extended H-rich CSM. Both the magnetar and CSM-interaction models of SN 2020zbf indicate that the progenitor mass at the time of explosion is between 2 and 5 M⊙. Modeling the spectral energy distribution of the host galaxy reveals a host mass of 108.7M⊙, a star formation rate of 0.24$ ^{+0.41}_{-0.12} $M⊙ yr–1, and a metallicity of ∼0.4 Z⊙.

Abstract Copyright: © The Authors 2024

Journal keyword(s): supernovae: general - supernovae: individual: SN 2020zbf

Simbad objects: 24

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Number of rows : 24
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 LSQ 12dlf SN* 01 50 29.80 -21 48 45.4           SLSN-I 57 0
2 SN 2020zbf SN* 01 58 01.650 -41 20 51.89           SLSN-I 3 0
3 PS1-10bzj SN* 03 31 39.826 -27 47 42.17           SLSN-I 55 0
4 AT 2020wnt SN? 03 46 37.950 +43 13 45.25           SNI 19 0
5 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
6 SN 2017gci SN* 06 46 45.02 -27 14 55.8           SLSN-I 23 0
7 PTF 10aagc SN* 09 39 56.923 +21 43 17.09           SLSN-I 30 0
8 SNLS 07D2bv SN* 10 00 06.62 +02 38 35.8           SLSN-I 27 0
9 SN 2017egm SN* 10 19 05.620 +46 27 14.08           SLSN-I 93 0
10 SN 2010gx SN* 11 25 46.71 -08 49 41.4           SLSN-I 165 1
11 SN 2015bn SN* 11 33 41.57 +00 43 32.2           SLSN-I 157 0
12 SN 2017ein SN* 11 52 53.26 +44 07 26.2           SNIc 69 0
13 SN 2016eay SN* 12 02 51.71 +44 15 27.4           SLSN-I 83 0
14 SN 2017ens SN* 12 04 09.36 -01 55 52.2           SLSN-I 43 0
15 SN 2007bi SN* 13 19 20.19 +08 55 44.3       18.3   SLSN-I 228 1
16 SN 2011ke SN* 13 50 57.77 +26 16 42.8     18.6     SLSN-I 92 1
17 PTF 12dam SN* 14 24 46.20 +46 13 48.3           SLSN-I 172 0
18 iPTF 13bvn SN* 15 00 00.152 +01 52 53.17           SNIb 211 0
19 SN 2018bsz SN* 16 09 39.110 -32 03 45.63           SNII 51 0
20 PTF 09cnd SN* 16 12 08.94 +51 29 16.1           SLSN-I 120 0
21 PTF 09atu SN* 16 30 24.55 +23 38 25.0           SLSN-I 63 0
22 SN 2010md SN* 16 37 47.00 +06 12 32.3           SLSN-I 110 1
23 iPTF 13ajg SN* 16 39 03.95 +37 01 38.4           SLSN-I 67 0
24 iPTF 16bad SN* 17 16 39.73 +28 22 12.6           SLSN-I 34 0

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