2017
DOI: 10.1093/mnras/stx1058
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Shaping planetary nebulae with jets in inclined triple stellar systems

Abstract: We conduct three-dimensional hydrodynamical simulations of two opposite jets launched obliquely to the orbital plane around an asymptotic giant branch (AGB) star and within its dense wind, and demonstrate the formation of a 'messy' planetary nebula (PN), namely, a PN lacking any type of symmetry (highly irregular). In building the initial conditions we assume that a tight binary system orbits the AGB star, and that the orbital plane of the tight binary system is inclined to the orbital plane of the binary syst… Show more

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Cited by 17 publications
(15 citation statements)
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“…Here we differ from the work of Akashi & Soker (2017) by launching the two opposite inclined jets inside the giant envelope, and we differ from our earlier simulation by injecting inclined jets and for a long time period. As we discuss below, we might as well refer to the orbital motion of the tight binary system in the outskirts of the giant envelope as a GEE (e.g., Shiber et al 2017;Shiber 2018).…”
Section: Introductioncontrasting
confidence: 76%
See 1 more Smart Citation
“…Here we differ from the work of Akashi & Soker (2017) by launching the two opposite inclined jets inside the giant envelope, and we differ from our earlier simulation by injecting inclined jets and for a long time period. As we discuss below, we might as well refer to the orbital motion of the tight binary system in the outskirts of the giant envelope as a GEE (e.g., Shiber et al 2017;Shiber 2018).…”
Section: Introductioncontrasting
confidence: 76%
“…In the present study we consider a tight binary system that enters the envelope of a giant star and experiences either a CEE or a grazing envelope evolution (GEE), or one after the other. We explore a new type of flow and base our simulation on two of our earlier studies, Akashi & Soker (2017) and Hillel et al (2017). Following a suggestion by Soker (2004), Akashi & Soker (2017) simulated the interaction of jets that a tight binary system launches into the wind of an AGB star.…”
Section: Introductionmentioning
confidence: 99%
“…Another setting is of the tight binary system that accretes mass from the wind of the AGB star, and one or two of the stars launch jets. When the inner orbital plane of the tight binary system is inclined to the orbital plane of the tight binary system around the AGB star, the morphology of the descendant PN might be lacking any type of symmetry (Soker 2004), i.e., be a 'messy PN' (highly irregular), as demonstrated by Akashi & Soker (2017). Soker (2004) listed several PNe that might have been shaped by a triple stellar progenitor, including IC 2149, NGC 6210, and NGC 1514 that we also mention in the present study.…”
Section: Introductionmentioning
confidence: 99%
“…Based on the nebular morphology, Bear & Soker (2017) classify Sh 2-71 as likely to have originated from a triple system, claiming that the pronounced lack of axial and/or mirror-symmetry is characteristic of such interactions. Furthermore, the hydrodynamical simulations of Akashi & Soker (2017) show that jets launched from a binary system in an inclined orbit with a tertiary AGB companion result in PN morphologies and density variations remarkably similar to those observed in Sh 2-71. This leads us to consider here the possibility that both binary A and star B form or once formed a triple system, the interacting evolution of which led to the formation of Sh 2-71.…”
Section: Introductionmentioning
confidence: 64%
“…The interactions within such a triple system as star B (the nebular progenitor in this scenario) lost its AGB envelope could feasibly have led to the formation of the unusual precessing disc found by Močnik et al (2015) in binary A. Similarly, mass transfer between star A and binary B could have led to the formation of jets (perhaps blown from the disc in binary A) which directly impacted upon the shaping of the nebula -leading to the "messy" morphology of the PN (considered to be a tell-tale sign of triple interactions; Akashi & Soker 2017;Bear & Soker 2017) as well as the observed shocks (Bohigas 2001). Furthermore, the newly identified extended emission regions, lying several arcminutes away from the centre of the PN but approximately aligned with the current positions of binary A and star B, may well be signposts of interactions within binary A or between binary A and the mass lost from star B during the PN formation episode.…”
Section: Discussionmentioning
confidence: 97%