Herschel HIFI observations of O$_2$ toward Orion: special conditions for shock enhanced emission
Jo-Hsin Chen, Paul F. Goldsmith, Serena Viti, Ronald Snell, Dariusz C., Lis, Arnold Benz, Edwin Bergin, John Black, Paola Caselli, Pierre Encrenaz,, Edith Falgarone, Javier R. Goicoechea, Ake Hjalmarson, David Hollenbach,, Michael Kaufman, Gary Melnick, David Neufeld

TL;DR
This study reports the detection of molecular oxygen emission in Orion, linking it to shock conditions and specific geometries that enhance O$_2$ abundance, explaining its rarity in other star-forming regions.
Contribution
It identifies the specific shock conditions and geometry that lead to enhanced O$_2$ emission in Orion, providing insights into molecular oxygen chemistry in star-forming regions.
Findings
O$_2$ detected at 487 GHz and 774 GHz, not at 1121 GHz.
O$_2$ emission region is ~9" near H2 Peak 1, not Peak A.
Enhanced O$_2$ abundance explained by low-velocity C-shock and UV radiation.
Abstract
We report observations of molecular oxygen (O) rotational transitions at 487 GHz, 774 GHz, and 1121 GHz toward Orion Peak A. The O2 lines at 487 GHz and 774 GHz are detected at velocities of 10-12 km/s with line widths 3 km/s; however, the transition at 1121 GHz is not detected. The observed line characteristics, combined with the results of earlier observations, suggest that the region responsible for the O emission is 9" (6e16 cm) in size, and is located close to the H2 Peak 1position (where vibrationally-excited H emission peaks), and not at Peak A, 23" away. The peak O2 column density is 1.1e18/cm2. The line velocity is close to that of 621 GHz water maser emission found in this portion of the Orion Molecular Cloud, and having a shock with velocity vector lying nearly in the plane of the sky is consistent with producing maximum maser gain along the line-of-sight. The…
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