Reverse shocks destroy small grains from supernovae, leaving mostly amorphous carbon and yielding flatter UV extinction curves consistent with high-redshift galaxy observations.
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Core-collapse supernovae create dust grains of many sizes in the first galaxies. The model follows how these grains grow or shrink over the first 30 million years in a star-forming burst, accounting for the reverse shock that sweeps back through the exploded material. This shock destroys nearly all grains smaller than 10 nanometers, leaving larger amorphous carbon grains as the main survivor. The resulting dust mixture absorbs and scatters ultraviolet light differently, producing a flatter attenuation curve with a wide bump near 2500 angstroms instead of the sharper features seen without shocks. The total dust mass relative to stars falls to about one ten-thousandth due to this destruction. These modeled curves and dust amounts line up with what JWST measures in distant galaxies.
Core claim
We find that our models are consistent with the observed attenuation curve and emissivity of high-redshift galaxies and show that the reverse shock processing significantly affects dust enrichment and grain properties such as extinction curves and emissivity in supernova yields for high-redshift galaxies.
Load-bearing premise
The assumption that a single starburst system with a standard initial mass function and varied but fixed progenitor parameters (rotation, metallicity, ISM density) accurately captures the conditions and dust processing in real high-redshift galaxies.
read the original abstract
Recent JWST observations have revealed that some galaxies at $z \gtrsim 7$ generally exhibit relatively flat ultraviolet (UV) attenuation curves and a weak UV bump. These features suggest that the first dust grains formed rapidly, possibly originating from core-collapse supernovae (SNe). We investigate the time evolution of grain size distributions and extinction curves in the early phase of dust enrichment for different parameters of progenitor stars, rotation velocities, metallicity, and interstellar medium densities, including the effect of the reverse shock. We model a single starburst system assuming an initial mass function. Extinction curves are calculated from the grain size distribution for each dust species. The total dust-to-stellar mass ratio at $30 \,\mathrm{Myr}$ is $M_\mathrm{dust}/M_\star \sim 10^{-3}$ before the passage of the reverse shock, but we find it to be at most $M_\mathrm{dust}/M_\star \sim 10^{-5}$ due to the destruction effect of the reverse shock. This effect destroys grains smaller than $\sim 10\,\mathrm{nm}$ and makes amorphous carbon the dominant species, resulting in a flatter extinction curve with a wide bump at $2500\,\mathrm{\mathring{A}}$ compared to the no-reverse shock models. We find that our models are consistent with the observed attenuation curve and emissivity of high-redshift galaxies and show that the reverse shock processing significantly affects dust enrichment and grain properties such as extinction curves and emissivity in supernova yields for high-redshift galaxies.
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The central claim rests on standard astrophysical assumptions about supernova dust formation and shock processing, with several free parameters varied to explore outcomes.
free parameters (2)
progenitor star parameters Rotation velocities, metallicities, and masses of progenitor stars are varied across models.
ISM density Interstellar medium densities are included as a variable parameter affecting grain evolution.
axioms (2)
domain assumptionStandard initial mass function governs the distribution of progenitor stars in the starburst system. Invoked to model the collective supernova contribution in a single starburst.
domain assumptionReverse shock destroys grains smaller than approximately 10 nm. Used to explain the shift to amorphous carbon dominance and flatter curves.
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