2021ApJ...921..180H


Query : 2021ApJ...921..180H

2021ApJ...921..180H - Astrophys. J., 921, 180-180 (2021/November-2)

Magnetar models of superluminous supernovae from the Dark Energy Survey: exploring redshift evolution.

HSU B., HOSSEINZADEH G. and BERGER E.

Abstract (from CDS):

Superluminous supernovae (SLSNe) are luminous transients that can be detected to high redshifts with upcoming optical time-domain surveys such as the Vera C. Rubin Observatory Legacy Survey of Space and Time. An interesting open question is whether the properties of SLSNe evolve through cosmic time. To address this question, in this paper we model the multicolor light curves of all 21 Type I SLSNe from the Dark Energy Survey (DES) with a magnetar spin-down engine, implemented in the Modular Open-Source Fitter for Transients (MOSFiT). With redshifts up to z ≃ 2, this sample includes some of the highest-redshift SLSNe. We find that the DES SLSNe span a similar range of ejecta and magnetar engine parameters as previous samples of mostly lower-redshift SLSNe (spin period P ≃ 0.79-13.61 ms, magnetic field B ≃ (0.03-7.33) x 1014 G, ejecta mass Mej ≃ 1.54-30.32 M☉, and ejecta velocity vej ≃ (0.55-1.45) x 104 km s–1). The DES SLSN sample by itself exhibits the previously found negative correlation between Mej and P, with a pronounced absence of SLSNe with low ejecta mass and rapid spin. Combining our results for the DES SLSNe with 60 previous SLSNe modeled in the same way, we find no evidence for redshift evolution in any of the key physical parameters.

Abstract Copyright: © 2021. The American Astronomical Society. All rights reserved.

Journal keyword(s): Supernovae

Simbad objects: 23

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Number of rows : 23
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 DES14E2slp SN* 00 33 04.08 -44 11 42.8           SLSN-I 5 0
2 DES15E2mlf SN* 00 41 33.40 -43 27 17.2           SLSN 17 0
3 DES15X1noe SN* 02 14 41.93 -04 52 54.5           SLSN-I 11 0
4 DES17X1amf SN* 02 17 46.70 -05 36 01.0           SLSN-I 13 0
5 DES17X1blv SN* 02 20 59.64 -04 29 00.8           SLSN-I 8 0
6 DES14X2byo SN* 02 23 46.93 -06 08 12.3           SLSN-I 13 0
7 DES15X3hm SN* 02 26 54.96 -05 03 38.0           SLSN-I 12 0
8 DES14X3taz SN* 02 28 04.46 -04 05 12.7           SLSN-I 47 0
9 DES15S2nr SN* 02 40 44.62 -00 53 26.4           SLSN-I 14 0
10 SN 2013hy SN* 02 42 32.82 -01 21 30.1           SLSN-I 35 1
11 DES14S2qri SN* 02 43 32.14 -01 07 34.2           SLSN-I 12 0
12 DES15S1nog SN* 02 52 14.98 -00 44 36.3           SLSN-I 9 0
13 DES16C3cv SN* 03 27 16.71 -28 42 45.9           SLSN-I 12 0
14 DES17C3gyp SN* 03 27 51.87 -28 23 44.3           SLSN-I 9 0
15 DES16C3ggu SN* 03 31 12.00 -28 34 38.7           SLSN-I 10 0
16 DES16C3dmp SN* 03 31 28.35 -28 32 28.3           SLSN-I 11 0
17 DES15C3hav SN* 03 31 52.17 -28 15 09.5           SLSN-I 17 0
18 DES14C1fi SN* 03 33 49.80 -27 03 31.6           SLSN-I 10 0
19 DES14C1rhg SN* 03 38 07.27 -27 42 45.7           SLSN-I 13 0
20 DES16C2nm SN* 03 40 14.83 -29 05 53.5           SLSN-I 17 0
21 DES16C2aix SN* 03 40 41.17 -29 22 48.4           SLSN-I 9 0
22 SN 2015bn SN* 11 33 41.57 +00 43 32.2           SLSN-I 157 0
23 SN 2006oz SN* 22 08 53.56 +00 53 50.4           SLSN-I 90 1

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