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VLTI-GRAVITY measurements of cool evolved stars

Daniel JadlovskýEuropean Southern Observatory (ESO)M. WittkowskiEuropean Southern Observatory (ESO)Andrea ChiavassaUniversité Côte d’Azur, Observatoire de la Côte d’Azur (OCA)Kateryna KravchenkoMax Planck Institute for Extraterrestrial Physics (MPE)B. FreytagTheoretical Astrophysics, Department of Physics and Astronomy, Uppsala UniversityS. HöfnerTheoretical Astrophysics, Department of Physics and Astronomy, Uppsala UniversityJiří KrtičkaDepartment of Theoretical Physics and Astrophysics, Faculty of Science, Masaryk UniversityClaudia PaladiniEuropean Southern Observatory (ESO)Gioia RauNational Science FoundationM. BrožCharles University, Faculty of Mathematics and Physics, Institute of AstronomyT. GranzerLeibniz-Institut für Astrophysik Potsdam (AIP)Michael WeberLeibniz-Institut für Astrophysik Potsdam (AIP)
2026en
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Aims . The mass-loss process of red supergiant (RSG) and asymptotic giant branch (AGB) stars and its relation to variability are poorly constrained. We aim to study the photosphere and near-surface atmospheric structure, where the mass-loss is initiated. For this purpose, we studied two oxygen-rich evolved stars: the Mira-type AGB star R Car and the RSG VX Sgr. Methods . We used the VLTI-GRAVITY instrument operating in the near-infrared K -band. Our sample comprises 54 VLTI-GRAVITY snapshots (18 R Car, 36 VX Sgr) taken over about 7 years, making it the largest VLTI time series dataset to date. We determined the angular diameter as a function of time for the continuum (photosphere) and selected atomic and molecular bands, i.e., lines of Ti I and Sc I as well as bands of H 2 O and CO. Furthermore, we compared the variability and atmospheric structure to state-of-the-art radiative-hydrodynamics CO5BOLD 3D simulations. Results . The radii of photosphere ( R ⋆ ) and extended atmospheric layers are variable and relate to the light curve with phase shifts. The near-photospheric layers show a maximum radius near visual brightness minima ( φ vis ∼ 0.4–0.6). Inner atomic (Ti I , Sc I ) and molecular (H 2 O) layers are further phase-shifted by ∆φ vis ~ 0.05. The more extended CO layers show longer, irregular periods and maximum extensions of ∼1.3–1.7 R ⋆ for R Car and of ∼1.5–2.2 R ⋆ for VX Sgr. Comparison with synthetic interferometric data of an AGB model based on several pulsation cycles in CO5BOLD simulations revealed a similar behavior. The photosphere shows regular pulsations, but with maximum diameters preceding minimum brightness ( φ vis < 0.5). The H 2 O layer showed a much weaker extension compared to our observations, while CO showed a good agreement. Furthermore, during the 2020–2021 season, VX Sgr exhibited an extreme mass-loss event similar to that of Betelgeuse, preceded by two strong shocks and culminating with the extreme expansion of H 2 O and CO layers, both up to ∼2.2 R ⋆ . Unexpectedly, during this event, we also detected Brackett γ in interferometric data as well as strong Balmer emission in optical spectra, both of which are also signatures of a shock propagating through the atmosphere. Conclusions . The Mira R Car showed an estimated photospheric radius of R ⋆ = 280 ± 25 R ⊙ , with a regular fundamental mode (FM) pulsation amplitude of ∼13% of R ⋆ . During its active cycle, the extreme RSG VX Sgr showed R ⋆ = 1556 ± 110 R e , with an FM pulsation amplitude of ∼13% of R ⋆ , the same as R Car. During its quiescent cycle, it showed a smaller value, R ⋆ = 1456 ± 108 R ⊙ , and low-amplitude pulsations near the first overtone (O1), only ∼4% of R ⋆ . This supports a steady mass-loss process for Mira stars related to stable large-amplitude FM pulsation, whereas the mass-loss process for RSGs may be dominated by extreme events connected to changes in the pulsation mode from low-amplitude O1 to large-amplitude FM pulsations.

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