2024Natur.627..754L


Query : 2024Natur.627..754L

2024Natur.627..754L - Nature, 627, 754-758 (2024/March-0)

A shock flash breaking out of a dusty red supergiant.

LI G., HU M., LI W., YANG Y., WANG X., YAN S., HU L., ZHANG J., MAO Y., RIISE H., GAO X., SUN T., LIU J., XIONG D., WANG L., MO J., ISKANDAR A., XI G., XIANG D., WANG L., SUN G., ZHANG K., CHEN J., LIN W., GUO F., LIU Q., CAI G., ZHOU W., ZHAO J., CHEN J., ZHENG X., LI K., ZHANG M., XU S., LYU X., CASTRO-TIRADO A.J., CHUFARIN V., POTAPOV N., IONOV I., KOROTKIY S., NAZAROV S., SOKOLOVSKY K., HAMANN N. and HERMAN E.

Abstract (from CDS):

Shock-breakout emission is light that arises when a shockwave, generated by the core-collapse explosion of a massive star, passes through its outer envelope. Hitherto, the earliest detection of such a signal was at several hours after the explosion, although a few others had been reported. The temporal evolution of early light curves should provide insights into the shock propagation, including explosion asymmetry and environment in the vicinity, but this has been hampered by the lack of multiwavelength observations. Here we report the instant multiband observations of a type II supernova (SN 2023ixf) in the galaxy M101 (at a distance of 6.85 ± 0.15 Mpc; ref. ), beginning at about 1.4 h after the explosion. The exploding star was a red supergiant with a radius of about 440 solar radii. The light curves evolved rapidly, on timescales of 1-2 h, and appeared unusually fainter and redder than predicted by the models within the first few hours, which we attribute to an optically thick dust shell before it was disrupted by the shockwave. We infer that the breakout and perhaps the distribution of the surrounding dust were not spherically symmetric.


Abstract Copyright: 2023 The Author(s), under exclusive licence to Springer Nature Limited

Journal keyword(s):

Simbad objects: 6

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Number of rows : 6
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 2016gkg SN* 01 34 14.46 -29 26 25.0           SNII 126 0
2 SN 2018zd SN* 06 18 03.180 +78 22 00.90           SNII 74 0
3 M 101 GiP 14 03 12.583 +54 20 55.50   8.46 7.86 7.76   ~ 3138 2
4 SN 2023ixf SN* 14 03 38.562 +54 18 41.94           SNII 209 0
5 SN 2013cu SN* 14 33 58.97 +40 14 20.7           SNII: 97 1
6 SN 2013fs SN* 23 19 44.70 +10 11 05.0           SNIIP 159 1

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