2025A&A...695A.271S


Query : 2025A&A...695A.271S

2025A&A...695A.271S - Astronomy and Astrophysics, volume 695A271 (2025/3-1)

The bright, dusty aftermath of giant eruptions and H-rich supernovae Late interaction of supernova shocks and dusty circumstellar shells created by 45, 50, and 60 M⊙ stars.

SERRANO-HERNANDEZ D.B., MARTINEZ-GONZALEZ S., JIMENEZ S., SILICH S. and WUNSCH R.

Abstract (from CDS):

Context. The late-stage evolution of massive stars is marked by periods of intense instability as they transit towards their final corecollapse. Within these periods, stellar eruptions stand out due to their hallmark of exceptionally high mass-loss rates, resulting in the formation of copious amounts of dust. However, the survival of these dust grains is threatened by the powerful shock waves generated when the progenitor star explodes as a supernova (SN).
Aims. We aim to assess the impact of selected cases of hydrogen-rich SN explosions from progenitors of 45, 50, and 60 M⊙ on dust grains formed after giant stellar eruptions, exploring late interactions with circumstellar shells that occur a few years to centuries after the eruption.
Methods. We present 3D hydrodynamical simulations that follow the evolution of dust particles in a scenario that includes, for the first time, the progenitor's stellar wind, a giant stellar eruption, and the eventual SN explosion, while in line with the mass budget prescribed by stellar evolutionary models.
Results. For a standard SN ejecta mass of 10 M⊙, kinetic energy of 1051 erg, and a long 200-year eruption-SN gap, only 25% of the dust mass remains 250 years post-explosion in a spherical circumstellar medium (CSM), and only 2% a century after the explosion in a bipolar CSM. Conversely, a shorter gap of a dozen years preserves 75% of the dust mass after shock-processing for a standard explosion, while this drops to 20% for more massive (15-20 M⊙) ejecta with kinetic energy of 5 × 1051 erg.
Conclusions. The CSM geometry and an early SN remnant transition to a radiative phase impact dust survival. As the shock wave weakens from efficiently converting kinetic energy into thermal radiation (up to half of the injected kinetic energy), there is a greater potential for survival, not only for dust in the CSM but also for SN-condensed dust (due to a weaker SN reverse shock), and pre-existing dust in the ambient ISM. Against expectations, a larger fraction of the dust mass can survive if the SN occurs just a few years after the eruption event.

Abstract Copyright: © The Authors 2025

Journal keyword(s): hydrodynamics - stars: massive - stars: mass-loss - supernovae: general - stars: winds, outflows - dust, extinction

Simbad objects: 14

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Number of rows : 14
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 SN 2005gl SN* 00 49 50.02 +32 16 56.8       17.0   SNIIn 162 2
3 SN 2013ej SN* 01 36 48.16 +15 45 31.0           SNIIP 248 0
4 SN 2005gj SN* 03 01 11.96 -00 33 13.9   18.6       SNIapec 209 1
5 SN 2006gy SN* 03 17 27.06 +41 24 19.5       14.20   SNIIn 372 1
6 SN 2018lab SN* 06 16 26.520 -21 22 32.38           SNII 19 0
7 SN 2016bse SN* 09 20 34.30 +50 41 46.8           SNIIP 134 0
8 SN 2005ip SN* 09 32 06.42 +08 26 44.4 18.1 18.7 18.5     SNIIn 230 1
9 NAME Homunculus Nebula ISM 10 45 03.5 -59 41 04           ~ 379 1
10 * eta Car s*b 10 45 03.545808 -59 41 03.95124 6.37 7.03 6.48 6.123 4.41 LBV 2543 0
11 SN 2015da SN* 13 52 24.16470 +39 41 27.9355           SNIIn 41 0
12 SN 2004dk SN* 16 21 48.93 -02 16 17.3   17.789 17.6     SNIb 98 1
13 SN 2004et SN* 20 35 25.33 +60 07 17.7   12.88       SNIIP 547 1
14 SN 2007od SN* 23 55 48.68 +18 24 54.8       14.4   SNIIP 147 1

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