The H2 Glow of a Quiescent Molecular Cloud Observed with JWST
We report JWST MIRI/MRS observations of the H _2 S (1) 17.04 μ m transition in two regions in the boundary of the Taurus molecular cloud. The two regions, denoted “Edge” (near the relatively sharp boundary of the ^13 CO J = 1 → 0 emission) and “Peak” (the location of the strongest H _2 emission obs...
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| Main Authors: | , , , , , , , , |
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| Format: | Article |
| Language: | English |
| Published: |
IOP Publishing
2025-01-01
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| Series: | The Astrophysical Journal Letters |
| Subjects: | |
| Online Access: | https://doi.org/10.3847/2041-8213/adcf9c |
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| Summary: | We report JWST MIRI/MRS observations of the H _2 S (1) 17.04 μ m transition in two regions in the boundary of the Taurus molecular cloud. The two regions, denoted “Edge” (near the relatively sharp boundary of the ^13 CO J = 1 → 0 emission) and “Peak” (the location of the strongest H _2 emission observed with Spitzer), have average intensities of 14.5 and 32.1 MJy sr ^−1 , respectively. We find small-scale structures of characteristic size 1 $\mathop{.}\limits^{\unicode{x02033}}$ 0–2 $\mathop{.}\limits^{\unicode{x02033}}$ 5, corresponding to 140–350 au, with characteristic intensity above the extended background of 10 MJy sr ^−1 , corresponding to a J = 3 column density of 1.6 × 10 ^17 cm ^−2 . The most plausible explanation for the observed intensities from this level 845 K above the J = 1 ortho-H _2 ground-state level is excitation by collisions with H _2 molecules (the hydrogen in this region being predominantly molecular). Two mechanisms, turbulent dissipation and shocks, have been proposed for the heating of localized regions of the interstellar medium (ISM) to temperatures ≃1000 K to explain abundances of and emission from particular molecules. While we cannot determine unique values of density and kinetic temperature, the solutions in best agreement with predictions of shock models are n (H _2 ) = 370 cm ^−3 and T _kin = 1000 K. The total H _2 column density of the small-scale structures under these conditions is ≃8 × 10 ^17 cm ^−2 . This first direct detection of significantly heated tiny-scale structures in the quiescent molecular ISM has significant implications for the physical structure of this phase of the ISM and the maintaining of supersonic motions within it. |
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| ISSN: | 2041-8205 |