2024ApJ...975..132S


Query : 2024ApJ...975..132S

2024ApJ...975..132S - Astrophys. J., 975, 132 (2024/November-1)

Unravelling the Asphericities in the Explosion and Multifaceted Circumstellar Matter of SN 2023ixf.

SINGH A., TEJA R.S., MORIYA T.J., MAEDA K., KAWABATA K.S., TANAKA M., IMAZAWA R., NAKAOKA T., GANGOPADHYAY A., YAMANAKA M., SWAIN V., SAHU D.K., ANUPAMA G.C., KUMAR B., ANCHE R.M., SANO Y., RAJ A., AGNIHOTRI V.K., BHALERAO V., BISHT D., BISHT M.S., BELWAL K., CHAKRABARTI S.K., FUJII M., NAGAYAMA T., MATSUMOTO K., HAMADA T., KAWABATA M., KUMAR A., KUMAR R., MALKAN B.K., SMITH P., SAKAGAMI Y., TAGUCHI K., TOMINAGA N. and WATANABE A.

Abstract (from CDS):

We present a detailed investigation of photometric, spectroscopic, and polarimetric observations of the Type II SN 2023ixf. Earlier studies have provided compelling evidence for a delayed shock breakout from a confined dense circumstellar matter (CSM) enveloping the progenitor star. The temporal evolution of polarization in the SN 2023ixf phase revealed three distinct peaks in polarization evolution at 1.4 days, 6.4 days, and 79.2 days, indicating an asymmetric dense CSM, an aspherical shock front and clumpiness in the low-density extended CSM, and an aspherical inner ejecta/He-core. SN 2023ixf displayed two dominant axes, one along the CSM-outer ejecta and the other along the inner ejecta/He-core, showcasing the independent origin of asymmetry in the early and late evolution. The argument for an aspherical shock front is further strengthened by the presence of a high-velocity broad absorption feature in the blue wing of the Balmer features in addition to the P-Cygni absorption post-16 days. Hydrodynamical light-curve modeling indicated a progenitor mass of 10M⊙ with a radius of 470 R⊙ and explosion energy of 2 × 1051 erg, along with 0.06 M⊙ of 56 Ni, though these properties are not unique due to modeling degeneracies. The modeling also indicated a two-zone CSM: a confined dense CSM extending up to 5 × 1014 cm with a mass-loss rate of 10–2M⊙ yr–1 and an extended CSM spanning from 5 × 1014 to at least 1016 cm with a mass-loss rate of 10–4M⊙ yr–1, both assuming a wind-velocity of 10 km s–1. The early-nebular phase observations display an axisymmetric line profile of [O I], redward attenuation of the emission of Hα post 125 days, and flattening in the Ks-band, marking the onset of dust formation.

Abstract Copyright: © 2024. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Core-collapse supernovae - Supernova dynamics - Type II supernovae - Red supergiant stars - Polarimetry - Spectropolarimetry

Status at CDS : Large table(s) will be appraised for possible ingestion in VizieR.

Simbad objects: 34

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Number of rows : 34
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 2017hcc SN* 00 03 50.580 -11 28 28.78           SNIIP 43 0
2 iPTF 13iqb SN* 00 34 04.84 -09 42 17.9           SNIIn 88 0
3 BD+64 106 ** 00 57 36.6894556320 +64 51 34.907455548 10.82 11.01   10.21   B1V 77 0
4 SN 2013ej SN* 01 36 48.16 +15 45 31.0           SNIIP 248 0
5 HD 236928 * 02 02 42.0929404728 +60 15 26.433482364   10.00 9.07     A4Ib 108 0
6 HD 14069 * 02 16 45.1936420248 +07 41 10.637150532   9.21 9.06     A0 61 0
7 SN 2017gmr SN* 02 35 30.15 -09 21 15.0           SNII 64 0
8 SN 2021yja SN* 03 24 21.180 -21 33 56.20           SNIIP 39 0
9 SN 2009ib SN* 04 17 40.09 -62 46 40.3           SNIIP 70 1
10 SN 1999em SN* 04 41 27.04 -02 51 45.2   13.79 13.7     SNIIP 727 1
11 SN 1987A SN* 05 35 27.98840 -69 16 11.1134           SNIIpec 5203 2
12 SN 2018zd SN* 06 18 03.180 +78 22 00.90           SNII 74 0
13 SN 2016gfy SN* 07 26 45.93 +85 45 51.2           SNII 18 0
14 2MASS J07371703+6535579 HXB 07 37 17.0432126424 +65 35 57.826001220           SNIIP 317 1
15 SN 2017ahn SN* 10 37 17.450 -41 37 05.27           SNII 54 0
16 SN 2012aw SN* 10 43 53.735 +11 40 17.63       15   SNIIP 252 1
17 SN 2014G SN* 10 54 34.13 +54 17 56.9           SNIIL 95 1
18 SN 1998S SN* 11 46 06.1 +47 28 55     12.2     SNIIn 517 1
19 PS1-13arp SN* 12 18 25.108 +46 37 01.30           SNIIP 14 0
20 SN 2020jfo SN* 12 21 50.480 +04 28 54.05           SNII 48 0
21 M 101 GiP 14 03 12.583 +54 20 55.50   8.46 7.86 7.76   ~ 3138 2
22 SN 2023ixf SN* 14 03 38.562 +54 18 41.94           SNII 209 0
23 NGC 5461 HII 14 03 40.96 +54 19 02.4           ~ 195 0
24 SN 2020tlf SN* 14 40 10.030 +42 46 39.64           SNII(n) 55 0
25 SN 2020pni SN* 15 03 49.960 +42 06 50.51           SNII 34 0
26 SN 2018gj SN* 16 32 02.31 +78 12 40.9           SNII 21 0
27 SN 2013by SN* 16 59 02.43 -60 11 41.8           SNII 83 1
28 HD 155528 * 17 12 19.9460340408 -04 24 09.248354532   10.08 9.60     B8Ib/II 34 0
29 BD+38 4058 EB* 20 23 28.5314538120 +39 20 59.037427788 12.02 11.81 10.62     B0V 69 0
30 SN 2017eaw SN* 20 34 44.238 +60 11 36.00           SNIIP 180 0
31 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
32 SN 2013fs SN* 23 19 44.70 +10 11 05.0           SNIIP 159 1
33 SN 2007od SN* 23 55 48.68 +18 24 54.8       14.4   SNIIP 147 1
34 SN 2008bk SN* 23 57 50.42 -32 33 21.5           SNIIP 167 2

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