2025ApJ...982L..32S


Query : 2025ApJ...982L..32S

2025ApJ...982L..32S - Astrophys. J., 982, L32 (2025/March-3)

Spectropolarimetry of SN 2023ixf Reveals Both Circumstellar Material and an Aspherical Helium Core.

SHRESTHA M., DeSOTO S., SAND D.J., WILLIAMS G.G., HOFFMAN J.L., SMITH P.S., McCALL C., MAUND J.R., STEELE I.A., WIERSEMA K., ANDREWS J.E., SMITH N., BILINSKI C., MILNE P., ANCHE R.M., BOSTROEM K.A., HOSSEINZADEH G., PEARSON J., LEONARD D.C., HSU B., DONG Y., HOANG E., JANZEN D., JENCSON J.E., JHA S.W., LUNDQUIST M.J., MEHTA D., MEZA RETAMAL N., VALENTI S., FARAH J., HOWELL D.A., McCULLY C., NEWSOME M., GONZALEZ E.P., PELLEGRINO C. and TERRERAN G.

Abstract (from CDS):

We present multi-epoch optical spectropolarimetric and imaging polarimetric observations of the nearby Type II supernova (SN) 2023ixf discovered in M101 at a distance of 6.85 Mpc. The first imaging polarimetric observations were taken +2.33 days (60085.08 MJD) after the explosion, while the last imaging polarimetric data points (+73.19 and +76.19 days) were acquired after the fall from the light-curve plateau. At +2.33 days there is strong evidence of circumstellar material (CSM) interaction in the spectra and the light curve. A significant level of intrinsic polarization pr = 1.02% ± 0.07% is seen during this phase, which indicates that this CSM is aspherical. We find that the polarization evolves with time toward the interstellar polarization level during the photospheric phase, which suggests that the recombination photosphere is spherically symmetric. There is a jump in polarization (pr = 0.45% ± 0.08% and pr = 0.62% ± 0.08%) at +73.19 and +76.19 days when the light curve falls from the plateau. This is a phase where polarimetric data are sensitive to nonspherical inner ejecta or a decrease in optical depth into the single-scattering regime. We also present spectropolarimetric data that reveal line (de)polarization during most of the observed epochs. In addition, at +14.50 days we see an “inverse P Cygni” profile in the H and He line polarization, which clearly indicates the presence of asymmetrically distributed material overlying the photosphere. The overall temporal evolution of the polarization is typical for Type II SNe, but the high level of polarization during the rising phase has only been observed in SN 2023ixf.

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

Journal keyword(s): Core-collapse supernovae - Type II supernovae - Red supergiant stars - Stellar mass loss - Circumstellar matter - Spectropolarimetry - Polarimetry

Simbad objects: 16

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Number of rows : 16
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 2013ej SN* 01 36 48.16 +15 45 31.0           SNIIP 248 0
2 SN 2017gmr SN* 02 35 30.15 -09 21 15.0           SNII 64 0
3 SN 2021yja SN* 03 24 21.180 -21 33 56.20           SNIIP 39 0
4 SN 1999em SN* 04 41 27.04 -02 51 45.2   13.79 13.7     SNIIP 727 1
5 2MASS J07371703+6535579 HXB 07 37 17.0432126424 +65 35 57.826001220           SNIIP 317 1
6 SN 2012aw SN* 10 43 53.735 +11 40 17.63       15   SNIIP 252 1
7 SN 2007aa SN* 12 00 27.69 -01 04 51.6 16.9 16.4 5.8     SNIIP 78 1
8 SN 2006ov SN* 12 21 55.30 +04 29 16.7     14.9     SNIIP 88 1
9 M 101 GiP 14 03 12.583 +54 20 55.50   8.46 7.86 7.76   ~ 3138 2
10 SN 2023ixf SN* 14 03 38.562 +54 18 41.94           SNII 209 0
11 HD 155528 * 17 12 19.9460340408 -04 24 09.248354532   10.08 9.60     B8Ib/II 34 0
12 BD+38 4058 EB* 20 23 28.5314538120 +39 20 59.037427788 12.02 11.81 10.62     B0V 69 0
13 Schulte 12 s*b 20 32 40.9572199728 +41 14 29.279036940 16.1 14.45 11.702     B3-4Ia+ 453 0
14 HD 340611 WD* 20 34 21.8847019255 +25 03 49.750446346 10.687 11.471 11.546 11.648 11.728 DA2.4 329 0
15 BD+28 4211 HS* 21 51 11.0221915656 +28 51 50.367627468 8.922 10.25 10.58 10.656 10.831 sdO2VIIIHe5 837 0
16 SN 2008bk SN* 23 57 50.42 -32 33 21.5           SNIIP 167 2

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