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

F. J. Ballieux, M. K. McClure, E. A. Bergin, M. L. R. Van 't Hoff, Ł. Tychoniec, L. Francis, E. F. Van Dishoeck
Original paper · DOI 10.3847/2041-8213/aebc81 Submitted to arXiv on 03 Nov. 2026 10 pages, 3 figures, 1 table. Accepted to the Astrophysical Journal Letters License: CC BY-NC-SA 4.0 Also in: fr

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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

  • 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 $1.1_{-0.1}^{+0.1}\times 10^{17}\,\rm{cm^{-2}}$.
  • 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.
  • 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.
  • 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.
  • 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.

AI-generated keywords: protoplanetary disks carbon chemistry disk winds JWST spectroscopy warm carbon-chain chemistry

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  • Original abstract
The paper investigates whether thermal processing of carbon-rich dust in a young protoplanetary disk can release carbon into the gas, potentially helping explain why Earth is so carbon-poor relative to the Sun. The authors study HOPS-68, a Class I protostar whose inner disk is thought to reach temperatures high enough to evaporate refractory material. They also explore how the observed hydrocarbons might form and whether carbon-chain chemistry usually attributed to warm carbon-chain chemistry (WCCC) could instead be linked to outflows. The team analyzes JWST Mid-Infrared Instrument spectra with local thermodynamic equilibrium absorption-slab models to estimate molecular temperatures, column densities, and velocities. They fit several bands individually or in combination, including features that overlap with water absorption. They also examine archival ALMA observations of C₂H, a molecule expected to form through ultraviolet processing of acetylene. Their interpretation builds on earlier work identifying a roughly 1,400 K inner-disk “thermostat” region and a warmer molecular layer associated with the base of a disk wind. The spectra show warm HCN and acetylene, with fitted temperatures of about 319 K and 432 K, respectively, and column densities of approximately 4.5 × 10¹⁷ and 1.1 × 10¹⁷ molecules per square centimeter. Their strongly blueshifted velocities—roughly 39–53 kilometers per second relative to the source—support an origin in the outflowing molecular layer. A second acetylene band yields a similar temperature, although some of its line parameters were fixed during fitting. The authors also report ¹³CCH₂, but the band is too faint for reliable modeling. Other detected species appear colder. The fitted temperatures are about 44 K for CH₃, 38 K for C₄H₂, and 54 K for CS. These molecules may be located in the upper outer disk, envelope, or outflow-cavity walls, but the data do not establish their locations. The study also reports a feature near 16.1 micrometers attributed to C₆H₂, described as the first detection of this species in a protostellar system. However, the authors could not model it because the necessary molecular data were unavailable. The identification is uncertain, as longer polyynes can have similar bending-mode wavelengths. A methane feature is also detected, but its inferred temperature is highly sensitive to continuum choices because it overlaps with other gas and ice features. The authors therefore do not rely on the fitted methane temperature. ALMA maps show C₂H emission extending along the outflow-cavity walls, with velocity structure consistent with outflowing rather than infalling gas. The authors propose that carbon-bearing material released from dust between roughly 500 K—the soot line—and about 1,200 K, where amorphous carbon can evaporate, is carried outward by a disk wind. In the cavity, ultraviolet light could convert acetylene into C₂H, which might then react with acetylene to form longer chains such as C₄H₂ and C₆H₂. The authors suggest that this process could contribute both to carbon loss from terrestrial planet-forming regions and to the aliphatic organic material found in meteorites and asteroids. They also propose that some polycyclic aromatic hydrocarbons (PAHs) might form through carbon combustion in the hot region, although they do not detect PAH emission in the on-source spectrum. These interpretations remain suggestive rather than established. The paper does not measure the wind’s total gas mass or quantify how much carbon it removes, and the proposed chemistry has not been confirmed through detailed modeling or spatially resolved observations of the longer carbon chains.

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