A Parsec-scale Circumstellar Shell Around VX Sgr: Mass Loss and RSG/T.ZO Nature
summary
The gist
The gist VX Sagittarii exhibits a thin, arc-shaped shell surrounding it, which suggests it is likely photoionized circumstellar material from past RSG wind or ejecta rather than a bow shock, and this
In short
The study discovered a thin, arc-shaped shell around VX Sagittarii (VX Sgr), suggesting it is photoionized circumstellar material from past RSG wind rather than a bow shock. This observation constrains VX Sgr to be an RSG/RHG, not a super-AGB star. The mass-loss rate is estimated at approximately 4 x 10^-5 M⊙ yr^-1, and future spectroscopic tests are needed to distinguish between RSG and Thorne–Zytkow Object (TZO) candidates.
Key concepts
- Circumstellar Shell
- A thin, arc-shaped structure surrounding a star like VX Sgr. It is thought to be photoionized material from the star's past wind, not shock heating. Its properties help determine the nature of the central star.
- RSG/RHG
- Red Supergiant or Red Hypergiant stars. VX Sgr is likely one of these types, as models suggest it is not compatible with super-AGB evolutionary tracks. This classification helps narrow down the star's physical properties and evolutionary stage.
- Mass-Loss Rate (M˙)
- The rate at which a star sheds its outer layers into space, measured in solar masses per year. The study estimates this rate to be around 4 x 10^-5 M⊙ yr^-1 based on the shell's geometry and ionizing radiation.
- Photoionization
- The process where ultraviolet light from a nearby star ionizes surrounding gas, creating a nebula. The arc shell is likely illuminated by an O- or B-type star, which provides the energy to excite the material.
Terminology used across episodes
This episode discusses
The paper
A Parsec-scale Circumstellar Shell Around VX Sgr: Mass Loss and RSG/T.ZO Nature · Read on arXiv
Julian Shapiro
Department of Astronomy, University of California, Berkeley
A thin, arc-shaped shell is discovered surrounding VX Sagittarii (VX Sgr), the largest known CSM shell around an RSG at a scale r about0.59, pc. The nebula has an extinction-corrected H α intensity I Hα about38, R and an ionized mass about0.1, M. The slow 12, km,s-1 peculiar velocity of VX Sgr and the lack of far-infrared emission in the arc indicate that it is not produced by a bow shock, but is likely instead steady RSG wind or ejecta that is photoionized by a nearby O - or B - type star. The nature of VX Sgr is debated in the literature as a red supergiant/hypergiant (RSG/RHG), super-AGB star, or Thorne--Żytkow Object (TŻO). Using the kinematic age of the Sgr OB1 association, the super-AGB model is disfavored. A spectroscopic test of the arc is proposed to potentially distinguish an RSG from a possible TŻO. The mass-loss rate is estimated from the geometry and emission measure of the shell, finding about4 times10-5, M, yr-1. The future interaction of the supernova (SN) ejecta of VX Sgr and the surrounding circumstellar material (CSM) is briefly explored through the mass ratio Λ of the shell and SN ejecta; the interaction would likely not have a significant effect on the SN forward shock.
Transcript
Introduction to the show: ident: Astrophysics Radio. Generated commentary on the latest astrophysics papers.
Vera: We're looking at the paper: "A Parsec-scale Circumstellar Shell Around VX Sgr".
Jocelyn: The gist VX Sagittarii exhibits a thin, arc-shaped shell surrounding it,
Vera: First, who's behind it and why it matters.
Title and authors: Vera: Let's talk about the title and authors for this paper, "A Parsec-scale Circumstellar Shell Around VX Sgr: Mass Loss and RSG/T.ZO Nature." It really tells you right away that they're focusing on the physical size of this shell—a parsec scale—and connecting it to the nature of the star itself.
Jocelyn: And looking at the authors, you've got Julian Shapiro and Daniel Jadlovský et al., which tells us we're looking at work coming from a team that’s deep into observational astronomy and spectral analysis.
Subrahmanyan: I see it as a paper trying to bridge the gap between what we observe in circumstellar material and the complex theoretical models of massive stellar evolution, specifically around red supergiants and hypergiants.
Vera: Basically, they're taking this one object, VX Sgr, which is already known for having a large shell, and using that shell's properties—like its arc shape—to argue whether it fits the standard picture of an RSG or if it might be something more exotic like a TZO.
Jocelyn: It’s interesting because the paper notes that the super-AGB model is disfavored by the kinematic age of that Sgr OB1 association, which sets a good baseline for how old this system is.
Subrahmanyan: That's crucial because if you can't fit it into one of these standard evolutionary tracks, it pushes us to think about alternative physics or different stages in stellar death.
Vera: They also mention that the literature has been debating whether VX Sgr is an RSG/RHG, a super-AGB star, or a Thorne–Zytkow Object. This paper aims to use new data to settle that debate.
Jocelyn: And they suggest that the way they test this—through spectroscopy—is key because it looks for specific spectral lines that might be unique to one class over the other.
The paper's summary: Vera: So, looking at the summary of "A Parsec-scale Circumstellar Shell Around VX Sgr: Mass Loss and RSG/T.ZO Nature," they detail how they characterized this thin arc-shaped shell around VX Sgr, noting its extinction-corrected H-alpha intensity is about thirty-eight R and its ionized mass is around zero point one solar masses.
Jocelyn: And the core finding here is that because of the slow peculiar velocity of twelve kilometers per second and no far-infrared emission in that arc, they conclude it's not a bow shock but steady RSG wind or ejecta being photoionized by a nearby O- or B-type star.
Subrahmanyan: That photoionization mechanism is important because it links the star to its immediate environment, suggesting an external influence rather than just internal stellar physics driving the shape of the shell.
Vera: They also explore how they estimate the mass-loss rate using geometry and emission measure, finding a value around four times ten to the minus five solar masses per year.
Jocelyn: That mass-loss rate estimate is interesting because it’s higher than what some other models predict for a star with that kind of brightness, which puts some pressure on the standard physics we use.
Subrahmanyan: And they are also exploring the ionization source, pointing to HD three hundred thirteen thousand eight hundred twenty-two as a strong candidate for being that nearby O- or B-type star ionizing the shell.
Vera: That connection between the shell and that specific star is what anchors their findings in reality, though they note their distance measurements to HD three hundred thirteen thousand eight hundred twenty-two are not precise enough to determine a separation.
The paper's improvements: Jocelyn: Moving on to the proposed improvements in "A Parsec-scale Circumstellar Shell Around VX Sgr: Mass Loss and RSG/T.ZO Nature," the authors suggest doing a spectroscopic test of that arc structure to potentially distinguish between an RSG and a possible TZO.
Vera: That sounds like they want to use spectroscopy to look for specific spectral lines that might be unique to an RSG versus a TZO, which is what they call a hypothetical star proposed by K. S. Thorne and A. N. Zytkow in one thousand nine hundred seventy-seven.
Subrahmanyan: I think that test is important because it moves the argument beyond just the visual shape of the shell and gives us something more definitive about its classification, which is what we need for better models of massive star evolution, especially for those nearing their end.
Jocelyn: They also discuss estimating the mass-loss rate by testing different wind structures, comparing an approximately constant wind to a distinct ejection episode.
Vera: That's a smart way to approach it because if they can find spectroscopic velocity measurements that distinguish between those two scenarios, it gives us more control over how we interpret the mass loss history.
Subrahmanyan: And thinking about the larger picture, this is about refining our models for those massive stars by seeing if the shell structure implies a steady wind or something more episodic.
Conclusion: Vera: The finding that VX Sgr is not compatible with the super-AGB evolutionary track is important because it helps us refine our models for those very massive stars that are nearing their end of their lives.
Subrahmanyan: I think that test is important because it moves the argument beyond just the visual shape of the shell and gives us something more definitive about its classification.
Vera: And they also briefly look at how future supernova ejecta from VX Sgr will interact with this shell, and they suggest that for a small mass ratio of shell to supernova ejecta, the effect of the circumstellar material on the supernova shock might not be significant.
Jocelyn: They also propose that these large-scale CSM structures surrounding VX Sgr and NML Cyg could represent an emerging class of extensive photoionized RSG shells, which is a big idea for us to keep watching.
Subrahmanyan: So, in short, this paper gives us constraints on the physical nature of VX Sgr through its shell structure and mass loss rate estimates.
Vera: That's the main point we are taking away from this work on "A Parsec-scale Circumstellar Shell Around VX Sgr: Mass Loss and RSG/T.ZO Nature."
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