2019
DOI: 10.1093/mnras/stz257
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A highly collimated jet from the Red Square nebula MWC 922

Abstract: Deep, narrow-band Hα and 6584Å [Nii] CCD images of the peculiar, infrared excess B[e] star MWC 922 reveal a collimated, bipolar jet orthogonal to the previously detected extended nebula. The jet consists of a pair of ∼0.15 pc segments on either side of MWC 922 separated by gaps. The most distant jet segments disappear ∼0.6 pc from the star. The northwest beam points to a faint emission-line feature 1.65 pc from MWC 922 that may be a terminal bow shock where the jet rams the ambient medium. The narrow opening-a… Show more

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Cited by 5 publications
(9 citation statements)
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“…Adopting an average H 2 density of ≈10 4 -10 5 cm −3 in the hot CO emitting region and using the column density estimated by Wehres et al (2017) we deduce that the size of the intervening CO-emitting region along the line of sight is probably Δ r ≈1-10 au. Note that the density of the hot CO-emitting gas is plausibly intermediate between that in the central H ii region studied here (~10 6 -10 7 cm −3 , § 4) and that of the more extended surrounding nebulosity traced by numerous forbidden and permitted emission lines in the optical (in the range ≈10-10 4 cm −3 , see Wehres et al 2017; Bally & Chia 2019). If we assume that the hot CO gas is located in a hollow cylindrical structure with a representative inner radius of R , and a thickness (Δ r ) and a scale height h ~Δ r , then we deduce a total mass in this component of only MH2hot[107108]×R1000auMfalse⊙.…”
Section: Discussionmentioning
confidence: 60%
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“…Adopting an average H 2 density of ≈10 4 -10 5 cm −3 in the hot CO emitting region and using the column density estimated by Wehres et al (2017) we deduce that the size of the intervening CO-emitting region along the line of sight is probably Δ r ≈1-10 au. Note that the density of the hot CO-emitting gas is plausibly intermediate between that in the central H ii region studied here (~10 6 -10 7 cm −3 , § 4) and that of the more extended surrounding nebulosity traced by numerous forbidden and permitted emission lines in the optical (in the range ≈10-10 4 cm −3 , see Wehres et al 2017; Bally & Chia 2019). If we assume that the hot CO gas is located in a hollow cylindrical structure with a representative inner radius of R , and a thickness (Δ r ) and a scale height h ~Δ r , then we deduce a total mass in this component of only MH2hot[107108]×R1000auMfalse⊙.…”
Section: Discussionmentioning
confidence: 60%
“…However, we believe that values much larger than ≈1000 au are unlikely since it would imply that the hot CO emission is reaching to, and coexisting with, the less dense and relatively extended optical/NIR nebulosity where the gas is known to be atomic and begins to be dissociated/ionized by the external (ISM) UV radiation field (e.g. Tuthill & Lloyd 2007; Wehres et al 2017; Bally & Chia 2019). The CO-ring scale height, h , is also unlikely to be significantly larger than Δ r since a very long, thin-walled tubular structure would hardly remain stable.…”
Section: Discussionmentioning
confidence: 99%
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“…However, numerous observations report very ordered outflows, where the outflow axis is straight on parsec scales (e.g. Bally & Chia 2019). For theoretical astrophysics, it would be of great interest to have some observationally informed statistics of complex versus straight outflows as a benchmark for the simulations.…”
Section: Outflow Directionsmentioning
confidence: 99%