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Herschel/PACS far-IR spectral imaging of a jet from an intermediate mass protostar in the OMC-2 region

2016/08/17 by B. González-García, B. Gonzalez-Garcia, P. Manoj +13 · 1 citation
Chemistry · Physics and Astronomy · #Accretion (finance) #Astro and Planetary Science #Astrophysics and Star Formation Studies #Fullerene Chemistry and Applications #Jet (fluid) #Line (geometry) #Luminosity #Outflow #Protostar #Spectral line #astro-ph.GA #astro-ph.SR

paper · pdf · doi:10.1051/0004-6361/201527186

Accepted for publication in A & A

arxiv created 2016/08/17 · openalex publication_date 2016/08/19 · openalex created_date 2016/09/16 · arxiv updated 2016/12/07 · openalex updated_date 2026/08/05

Abstract

We present the first detection of a jet in the far-IR [O I] lines from an intermediate mass protostar. This jet was detected in a Herschel/PACS spectral mapping study in the [O I] lines of OMC-2 FIR 3 and FIR 4, two of the most luminous protostars in Orion outside of the Orion Nebula. The spatial morphology of the fine structure line emission reveals the presence of an extended photodissociation region (PDR) and a narrow, but intense jet connecting the two protostars. The jet seen in [O I] emission is spatially aligned with the Spitzer/IRAC 4.5 μm jet and the CO (6–5) molecular outflow centered on FIR 3. The mass-loss rate derived from the total [O I] 63 μm line luminosity of the jet is 7.7 × 10-6M⊙ yr-1, more than an order of magnitude higher than that measured for typical low-mass class 0 protostars. The implied accretion luminosity is significantly higher than the observed bolometric luminosity of FIR 4, indicating that the [O I] jet is unlikely to be associated with FIR 4. We argue that the peak line emission seen toward FIR 4 originates in the terminal shock produced by the jet driven by FIR 3. The higher mass-loss rate that we find for FIR 3 is consistent with the idea that intermediate-mass protostars drive more powerful jets than their low-mass counterparts. Our results also call into question the nature of FIR 4.

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