The Spectra of a Radiative Reprocessing Outflow Model for Fast Blue Optical Transients

Abstract The radiation reprocessing model, in which an optically thick outflow absorbs the high-energy emission from a central source and reemits in longer wavelengths, has been frequently invoked to explain some optically bright transients, such as fast blue optical transients (FBOTs), whose progenitor and explosion mechanism are still unknown. Previous studies on this model did not take into account the frequency dependence of the opacity. We study the radiative reprocessing and calculate the UV-optical-near-infrared (NIR) band spectra from a spherical outflow composed of pure hydrogen gas, for a time-dependent outflowing mass rate. Electron scattering and frequency-dependent bound–free and free–free opacities are considered. The spectrum deviates from the blackbody at NIR and UV frequencies; in particular, it has νL ν ∝ ν 1.5 at NIR frequencies, because at these frequencies the absorption optical depth from the outflow’s outer edge to the so-called photon trapping radius is large and is frequency dependent. We apply our model to the prototype FBOT AT2018cow by fitting the spectra to the observed spectral energy distribution. The best-fit mass-loss rate suggests that the total outflow mass in AT2018cow is <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mrow> <mml:mi>M</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">out</mml:mi> </mml:mrow> </mml:msub> <mml:mo>≈</mml:mo> <mml:mn>5</mml:mn> <mml:mo>.</mml:mo> <mml:msubsup> <mml:mrow> <mml:mn>7</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.4</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.4</mml:mn> </mml:mrow> </mml:msubsup> <mml:mspace width="0.25em"/> <mml:msub> <mml:mrow> <mml:mi>M</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>⊙</mml:mo> </mml:mrow> </mml:msub> </mml:math> . If that equals the total mass lost during an explosion, and if the progenitor is a blue supergiant (with a preexplosion mass of ∼20 M ⊙ ), then it will suggest that the central compact remnant mass is at least ≈14 M ⊙ . This would imply that the central remnant is a black hole.

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Publication Details

Journal
The Astrophysical Journal
Published
2025-09-26
DOI
https://doi.org/10.3847/1538-4357/ae0181
Citations
2
Primary Topic
Advanced Optical Sensing Technologies
Type
article
Field-Weighted Citation Impact
2.38
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article

The Spectra of a Radiative Reprocessing Outflow Model for Fast Blue Optical Transients

Rong-Feng Shen, Chun 春 Chen 陈
2 citations
The Astrophysical Journal
Advanced Optical Sensing Technologies
2.38
article

The Spectra of a Radiative Reprocessing Outflow Model for Fast Blue Optical Transients

Rong-Feng Shen, Chun 春 Chen 陈
article en
2 citations

Abstract

Abstract The radiation reprocessing model, in which an optically thick outflow absorbs the high-energy emission from a central source and reemits in longer wavelengths, has been frequently invoked to explain some optically bright transients, such as fast blue optical transients (FBOTs), whose progenitor and explosion mechanism are still unknown. Previous studies on this model did not take into account the frequency dependence of the opacity. We study the radiative reprocessing and calculate the UV-optical-near-infrared (NIR) band spectra from a spherical outflow composed of pure hydrogen gas, for a time-dependent outflowing mass rate. Electron scattering and frequency-dependent bound–free and free–free opacities are considered. The spectrum deviates from the blackbody at NIR and UV frequencies; in particular, it has νL ν ∝ ν 1.5 at NIR frequencies, because at these frequencies the absorption optical depth from the outflow’s outer edge to the so-called photon trapping radius is large and is frequency dependent. We apply our model to the prototype FBOT AT2018cow by fitting the spectra to the observed spectral energy distribution. The best-fit mass-loss rate suggests that the total outflow mass in AT2018cow is <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mrow> <mml:mi>M</mml:mi> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">out</mml:mi> </mml:mrow> </mml:msub> <mml:mo>≈</mml:mo> <mml:mn>5</mml:mn> <mml:mo>.</mml:mo> <mml:msubsup> <mml:mrow> <mml:mn>7</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.4</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.4</mml:mn> </mml:mrow> </mml:msubsup> <mml:mspace width="0.25em"/> <mml:msub> <mml:mrow> <mml:mi>M</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>⊙</mml:mo> </mml:mrow> </mml:msub> </mml:math> . If that equals the total mass lost during an explosion, and if the progenitor is a blue supergiant (with a preexplosion mass of ∼20 M ⊙ ), then it will suggest that the central compact remnant mass is at least ≈14 M ⊙ . This would imply that the central remnant is a black hole.

The Astrophysical JournalVol. 991(2)
Openalex Percentile: Top 10%
Advanced Optical Sensing Technologies
2.38
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