AI summary · arXiv: 2611.04557v1 · astro-ph.SR
Up in smoke: carbon-destruction in the terrestrial planet-forming region of a young Class I disk
The essentials
JWST and ALMA observations of HOPS-68 reveal warm carbon-bearing gas in a disk wind and colder carbon chains near outflow cavity walls, motivating a proposed route for carbon redistribution and chain formation.
Question
What is the origin and location of the diverse hydrocarbons observed around the young Class I protostar HOPS-68? The authors assess whether thermal release of carbon in the inner disk, followed by transport and chemistry in outflows, could help explain terrestrial carbon depletion and the observed carbon chains.
Method
The authors analyzed JWST/MIRI absorption bands with LTE slab models to estimate molecular temperatures, column densities, and velocities, using Bayesian fitting; the JWST exposure totaled 222 seconds. They also examined archival ALMA band 6 C2H observations at 262.065 GHz to map its emission relative to the H2 jet and outflow cavity.
Findings
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Result
The slab fits yield warm HCN and C2H2, with temperatures of 319 K and 432 K and column densities of 4.5 × 10^17 cm−2 and 1.1 × 10^17 cm−2, respectively.
See the passage in the paper
The best-fitting slab model for HCN returns a temperature of $319_{-24}^{+22}$ K and a column density of $4.5_{-0.7}^{+1.1}\times 10^{17}\,\rm{cm^{-2}}$. The $\rm{C_{2}H_{2}}$ is best fit by a slab model with a temperature of $432_{-16}^{+15}$ K and a column density of $1.1_{-0.1}^{+0.1}\times 10^{17}\,\rm{cm^{-2}}$.
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Authors’ interpretation
The warm HCN and C2H2 are strongly blueshifted, and the authors associate them with the same warm molecular layer as oxygen-bearing species at the base of the disk wind.
See the passage in the paper
The temperatures of HCN and $\rm{C_{2}H_{2}}$ (between $319$ and $432\,\rm{K}$) and blue-shifted velocities (by between $53$ and $39\,\rm{km\,s^{-1}}$ with respect to the source velocity), are similar to those found in paper A for the oxygen-bearing species, so we conclude that these hydrocarbons are in the same molecular layer.
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Result
CH3, C4H2, and CS have fitted temperatures near 40–54 K, while C6H2 is detected but cannot be reliably fitted with the slab models.
See the passage in the paper
With temperatures of $44_{-7}^{+7}\,\rm{K}$ and $38_{-11}^{+12}\,\rm{K}$ respectively, these hydrocarbons are relatively cold.
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Authors’ interpretation
ALMA C2H emission brackets the H2 jet and is interpreted as tracing outflowing material along the cavity walls rather than infalling material.
See the passage in the paper
These clearly bracket the JWST/MIRI observations of the $\rm{H_{2}\,S(3)}$ jet, indicating that $\rm{C_{2}H}$ traces a wider component than the jet, likely the outflow cavity walls. Furthermore, the blue-shift of the $\rm{C_{2}H}$ emission follows that of the jet, indicating that it traces outflowing, rather than infalling, material.
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Authors’ interpretation
The authors propose that carbon released from grains in an inner-disk destruction zone is carried outward by the disk wind, while UV-driven reactions in the cavity walls can form longer carbon chains.
See the passage in the paper
We suggest that the warm simple hydrocarbons such as $\rm{C_{2}H_{2}}$ sublimate from dust grains in a "refractory grain destruction zone" in the inner disk, and are subsequently entrained in the disk wind.
Limitations
- The study does not quantify how much carbon the disk wind removes or how much this could contribute to Earth's carbon depletion; that analysis is left for future work.
See the passage in the paper
To constrain the amount of carbon carried off in the wind, and to estimate its contribution to the abundances observed on Earth, we would have to quantitatively constrain the amount of gas in the disk wind, using e.g. the IR $\rm{H_{2}}$ lines or mm CO observations. Such an analysis is outside of the scope of this letter, but will be done in future work.
- The proposed cavity-wall carbon-chain formation pathway is not confirmed, and the authors call for larger-scale observations and chemical modeling.
See the passage in the paper
To determine whether the observed carbon chain species are indeed formed through UV-induced chemistry in the outer disk or envelope, we would need larger-scale (sub)-mm observations of carbon-chain species, to see if their location coincides with the observed $\rm{C_{2}H}$ emission.
- The CH4 fit is not robust because overlapping features and continuum choices allow a wide range of fitted temperatures.
See the passage in the paper
Varying the continuum subtraction allowed us to fit a large range of temperatures (between $\sim$ 10 and 1000 K) to the band, indicating that the fitting results from this band are not robust.
Why it matters
The authors argue that inner-disk thermal processing and winds may provide a mechanism contributing to carbon depletion in terrestrial planet-forming material. They also propose that some carbon-chain chemistry attributed to infalling-envelope WCCC may instead occur in outflow cavity walls, with possible relevance to aliphatic organics in meteorites and asteroids.
Written by AI from the paper. Passages are checked word for word against the text we analysed; the rest may contain errors.
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