2021MNRAS.503..312M


Query : 2021MNRAS.503..312M

2021MNRAS.503..312M - Mon. Not. R. Astron. Soc., 503, 312-323 (2021/May-1)

RINGO3 polarimetry of very young ZTF supernovae.

MAUND J.R., YANG Y., STEELE I.A., BAADE D., JERMAK H., SCHULZE S., BRUCH R., GAL-YAM A., HOFLICH P.A., OFEK E., WANG X., AMENOUCHE M., DEKANY R., MASCI F.J., RIDDLE R. and SOUMAGNAC M.T.

Abstract (from CDS):

The early phases of the observed evolution of the supernovae (SNe) are expected to be dominated by the shock breakout and 'flash' ionization of the surrounding circumstellar medium. This material arises from the last stages of the evolution of the progenitor, such that photometry and spectroscopy of SNe at early times can place vital constraints on the latest and fastest evolutionary phases leading up to stellar death. These signatures are erased by the expansion of the ejecta within ∼5 d after explosion. Here we present the earliest constraints, to date, on the polarization of 10 transients discovered by the Zwicky Transient Facility (ZTF), between 2018 June and 2019 August. Rapid polarimetric follow-up was conducted using the Liverpool Telescope RINGO3 instrument, including three SNe observed within <1 d of detection by the ZTF. The limits on the polarization within the first 5 d of explosion, for all SN types, is generally < 2 per cent, implying early asymmetries are limited to axial ratios >0.65 (assuming an oblate spheroidal configuration). We also present polarimetric observations of the Type I Superluminous SN 2018bsz and Type II SN 2018hna, observed around and after maximum light.

Abstract Copyright: © 2021 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): techniques: polarimetric - supernovae: general

Simbad objects: 25

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Number of rows : 25
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 BD+64 106 ** 00 57 36.6894556320 +64 51 34.907455548 10.82 11.01   10.21   B1V 77 0
2 HD 236928 * 02 02 42.0929404728 +60 15 26.433482364   10.00 9.07     A4Ib 108 0
3 SN 2018gvi SN* 02 55 36.00 +43 03 27.3           SN.Ia 4 0
4 HD 283812 * 04 44 24.9210299331 +25 31 42.390958427   10.24 9.5     A2 55 0
5 SN 1987A SN* 05 35 27.98840 -69 16 11.1134           SNIIpec 5203 2
6 SN 2019np SN* 10 29 21.980 +29 30 38.30           SNIa 50 0
7 SN 2015bn SN* 11 33 41.57 +00 43 32.2           SLSN-I 157 0
8 SN 1998S SN* 11 46 06.1 +47 28 55     12.2     SNIIn 517 1
9 SN 2018hna SN* 12 26 12.070 +58 18 50.83           SNII 16 0
10 SN 2019ein SN* 13 53 29.13 +40 16 31.3           SNIa 38 0
11 SN 2013cu SN* 14 33 58.97 +40 14 20.7           SNII: 97 1
12 SN 2018cyg SN* 15 34 08.480 +56 41 48.73           SNII 7 0
13 SN 2019hgp SN* 15 36 12.90 +39 44 00.6           SNIcn 29 0
14 SN 2018bsz SN* 16 09 39.110 -32 03 45.63           SNII 51 0
15 SN 2018gep SN* 16 43 48.2 +41 02 43           SNIc-BL 66 0
16 SN 2018dfi SN* 16 50 50.10 +45 23 52.5           SN.II 8 0
17 SN 2018cnw SN* 16 59 05.07 +47 14 11.1           SNIa 19 0
18 HD 155528 * 17 12 19.9460340408 -04 24 09.248354532   10.08 9.60     B8Ib/II 34 0
19 MCG+10-25-029 AG? 17 25 38.42 +59 26 48.4   16.5       ~ 27 0
20 SN 2019nvm SN* 17 25 38.667 +59 26 48.26           SN.II 11 0
21 SN 2018eay SN* 18 16 13.10 +55 35 27.2           SNIa-91T-like 11 0
22 BD+38 4058 EB* 20 23 28.5314538120 +39 20 59.037427788 12.02 11.81 10.62     B0V 69 0
23 Schulte 12 s*b 20 32 40.9572199728 +41 14 29.279036940 16.1 14.45 11.702     B3-4Ia+ 453 0
24 SN 2009ip s*b 22 23 08.26 -28 56 52.4           LBV 406 0
25 HD 215806 * 22 46 40.2387415872 +58 17 43.950809976 9.05 9.52 9.23     O 58 0

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