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Velocity-resolved [C II] Emission and [C II]/FIR mapping along Orion with Herschel

AutorGoicoechea, Javier R. CSIC ORCID; Teyssier, D.; Etxaluze, Mireya; Goldsmith, P. F.; Ossenkopf-Okada, V.; Gerin, M.; Bergin, E. A.; Black, J. H.; Cernicharo, José CSIC ORCID ; Cuadrado, Sara CSIC ORCID; Encrenaz, P.; Falgarone, E.; Fuente, A.; Hacar, A.; Lis, D.C.; Marcelino, Nuria CSIC ORCID; Melnick, Gary J.; Müller, H. S. P.; Persson, C.; Pety, J.; Röllig, M.; Schilke, P.; Simon, R.; Snell, R. L.; Stutzki, J.
Palabras claveGalaxies: ISM
ISM: clouds
Infrared: galaxies
H ii regions
Fecha de publicación9-oct-2015
EditorIOP Publishing
CitaciónAstrophysical Journal 812(1): 75 (2015)
ResumenWe present the first ∼7.′5 11.′5 velocity-resolved (∼0.2 km s) map of the [C ii] 158 μm line toward the Orion molecular cloud 1 (OMC 1) taken with the Herschel/HIFI instrument. In combination with far-IR (FIR) photometric images and velocity-resolved maps of the H41α hydrogen recombination and CO J = 2-1 lines, this data set provides an unprecedented view of the intricate small-scale kinematics of the ionized/photodissociation region (PDR)/molecular gas interfaces and of the radiative feedback from massive stars. The main contribution to the [C ii] luminosity (∼85%) is from the extended, FUV-illuminated face of the cloud (G > 500, 5 10 cm) and from dense PDRs ( 10, 10 cm) at the interface between OMC 1 and the H ii region surrounding the Trapezium cluster. Around ∼15% of the [C ii] emission arises from a different gas component without a CO counterpart. The [C ii] excitation, PDR gas turbulence, line opacity (from [C ii]), and role of the geometry of the illuminating stars with respect to the cloud are investigated. We construct maps of the L[C ii]/ and / ratios and show that L[C ii]/ decreases from the extended cloud component (∼10-10) to the more opaque star-forming cores (∼1010). The lowest values are reminiscent of the >[C ii] deficit> seen in local ultraluminous IR galaxies hosting vigorous star formation. Spatial correlation analysis shows that the decreasing L[C ii]/ ratio correlates better with the column density of dust through the molecular cloud than with /. We conclude that the [C ii]-emitting column relative to the total dust column along each line of sight is responsible for the observed L[C ii]/ variations through the cloud.
Versión del editorhttps://doi.org/10.1088/0004-637X/812/1/75
URIhttp://hdl.handle.net/10261/183080
DOI10.1088/0004-637X/812/1/75
Identificadoresdoi: 10.1088/0004-637X/812/1/75
e-issn: 1538-4357
issn: 0004-637X
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