The Optical to X-Ray Luminosity and Spectrum of Supernova Wind Breakouts

Abstract Observations indicate that an optically thick circumstellar medium (CSM) at radii of 10 14 –10 15 cm around Type II core-collapse supernova (SN) progenitors is common (and may be present in other types of massive star explosions). The breakout of the SN radiation-mediated shock (RMS) through such a CSM leads to the formation of a collisionless shock (CLS). We analyze the evolution of the shock structure and associated radiation field during and after the RMS–CLS transition for nonrelativistic shock breakout velocities ( v bo = 10 9 v 9 cm s −1 &lt; 0.1 c ) through a hydrogen-rich CSM “wind” density profile, ρ ∝ r −2 , with breakout radius R bo = 10 14 R 14 cm, much larger than the progenitor radius. An analytic description of the key properties of the emitted optical to X-ray radiation is provided, supported by numeric radiation hydrodynamics calculations self-consistently describing the time-dependent spatial distribution of the plasma and radiation, governed by bremsstrahlung emission/absorption and inelastic Compton scattering. The characteristic energy of the photons carrying most of the luminosity, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mo>≈</mml:mo> <mml:mn>1</mml:mn> <mml:msup> <mml:mn>0</mml:mn> <mml:mn>43</mml:mn> </mml:msup> <mml:mspace width="0.25em"/> <mml:msub> <mml:mi>R</mml:mi> <mml:mn>14</mml:mn> </mml:msub> <mml:mspace width="0.25em"/> <mml:msubsup> <mml:mi>v</mml:mi> <mml:mn>9</mml:mn> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mspace width="1em"/> </mml:math> erg s −1 , shifts from UV to X-rays, reaching 1 keV as the shock reaches ≈3 R bo , in ≈3 R 14 / v 9 days. The X-ray signal is not suppressed by propagation through the upstream wind, and its absence may suggest that the dense CSM does not extend much beyond R bo . Our results provide the basis for a quantitative calculation of the high-energy γ -ray and neutrino emission that is expected from particles accelerated at the CLS, and will allow using data from upcoming surveys that will systematically detect large numbers of young SNe, particularly ULTRASAT, to infer the preexplosion mass-loss history of the SN progenitor population.

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Publication Details

Journal
The Astrophysical Journal
Published
2025-10-23
DOI
https://doi.org/10.3847/1538-4357/adfecc
Citations
2
Primary Topic
Gamma-ray bursts and supernovae
Type
article
Field-Weighted Citation Impact
2.31
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article

The Optical to X-Ray Luminosity and Spectrum of Supernova Wind Breakouts

Péter Szabó, Eli Waxman, Nir Sapir, T. Wasserman
2 citations
The Astrophysical Journal
Gamma-ray bursts and supernovae
2.31
article

The Optical to X-Ray Luminosity and Spectrum of Supernova Wind Breakouts

Péter Szabó, Eli Waxman, Nir Sapir, T. Wasserman
article en
2 citations

Abstract

Abstract Observations indicate that an optically thick circumstellar medium (CSM) at radii of 10 14 –10 15 cm around Type II core-collapse supernova (SN) progenitors is common (and may be present in other types of massive star explosions). The breakout of the SN radiation-mediated shock (RMS) through such a CSM leads to the formation of a collisionless shock (CLS). We analyze the evolution of the shock structure and associated radiation field during and after the RMS–CLS transition for nonrelativistic shock breakout velocities ( v bo = 10 9 v 9 cm s −1 &lt; 0.1 c ) through a hydrogen-rich CSM “wind” density profile, ρ ∝ r −2 , with breakout radius R bo = 10 14 R 14 cm, much larger than the progenitor radius. An analytic description of the key properties of the emitted optical to X-ray radiation is provided, supported by numeric radiation hydrodynamics calculations self-consistently describing the time-dependent spatial distribution of the plasma and radiation, governed by bremsstrahlung emission/absorption and inelastic Compton scattering. The characteristic energy of the photons carrying most of the luminosity, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mo>≈</mml:mo> <mml:mn>1</mml:mn> <mml:msup> <mml:mn>0</mml:mn> <mml:mn>43</mml:mn> </mml:msup> <mml:mspace width="0.25em"/> <mml:msub> <mml:mi>R</mml:mi> <mml:mn>14</mml:mn> </mml:msub> <mml:mspace width="0.25em"/> <mml:msubsup> <mml:mi>v</mml:mi> <mml:mn>9</mml:mn> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mspace width="1em"/> </mml:math> erg s −1 , shifts from UV to X-rays, reaching 1 keV as the shock reaches ≈3 R bo , in ≈3 R 14 / v 9 days. The X-ray signal is not suppressed by propagation through the upstream wind, and its absence may suggest that the dense CSM does not extend much beyond R bo . Our results provide the basis for a quantitative calculation of the high-energy γ -ray and neutrino emission that is expected from particles accelerated at the CLS, and will allow using data from upcoming surveys that will systematically detect large numbers of young SNe, particularly ULTRASAT, to infer the preexplosion mass-loss history of the SN progenitor population.

The Astrophysical JournalVol. 993(1)
Israel Atomic Energy Commission (IL), Soreq Nuclear Research Center, Weizmann Institute of Science (IL)
Openalex Percentile: Top 10%
Gamma-ray bursts and supernovae
2.31
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