4.6 Article

Extending the FIP bias sample to magnetically active stars Challenging the FIP bias paradigm

期刊

ASTRONOMY & ASTROPHYSICS
卷 659, 期 -, 页码 -

出版社

EDP SCIENCES S A
DOI: 10.1051/0004-6361/202141493

关键词

stars; abundances; stars; activity; stars; atmospheres

资金

  1. Hungarian National Research, Development and Innovation Office grants NKFIH (OTKA) [K-131508, KH-130526, NN129075, K129249]
  2. NKFIH grant [2019-2.1.11-TET-2019-00056]
  3. Austrian-Hungarian Action Foundation [101ou13, 104ou2]
  4. Hungarian National Research, Development and Innovation Office [NKFIH PD-134784]
  5. NASA [80HQTR19T0029, 80HQTR20T0076]
  6. Basic Research FUnds of the Office of Naval Research
  7. STFC [ST/S000240/1]

向作者/读者索取更多资源

The different elemental abundances of the photosphere and the corona in the Sun and other stars are influenced by the first ionisation potential (FIP) effect, which is characterized by the FIP bias. This study investigates the relationship between the surface temperature of stars and the FIP bias, as well as the influence of other astrophysical parameters. The results show that there are new features in the T-eff-FIP bias diagram, and the FIP bias is influenced by stellar activity indicators and other parameters. The study also identifies three clusters in the FIP bias determinant parameter space.
Context. The different elemental abundances of the photosphere and the corona are striking features of not only the Sun, but of other stars as well. This phenomenon is known as the first ionisation potential (FIP) effect, and its strength can be characterized by the FIP bias, the logarithmic abundance difference between low- and high-FIP elements in the corona, compared to the photosphere. The FIP bias was shown to depend on the surface temperature of the star. Aims. We aim to extend the T-eff-FIP bias relationship to a larger stellar sample and analyse the effect of other astrophysical parameters on the relation (e.g. surface gravity, age, activity indicators). Methods. We compiled FIP bias and other parameters for 59 stars for which coronal composition is available, now including evolved stars. Using principal component analysis and linear discriminant analysis, we searched for correlations with other astrophysical parameters within the sample that may influence the stellar FIP bias. Results. Adding stars to the T-eff-FIP bias diagram unveiled new features in its structure. In addition to the previously known relationship, there appears to be a second branch: a parallel sequence about 0.5 dex above it. While the T-eff remains the main determinant of the FIP bias, other parameters such as stellar activity indicators also have influence. We find three clusters in the FIP bias determinant parameter space. One distinct group is formed by the evolved stars. Two groups contain main sequence stars in continuation separated roughly by the sign change of the FIP-bias value. Conclusions. The new branch of the T-eff-FIP bias diagram contains stars with higher activity level, in terms of X-ray flux and rotational velocity. The Rossby number also seems to be important, indicating possible dependence on the type of dynamo operating in these stars influencing their FIP bias. The two main-sequence clusters run from the earliest spectral types of A-F with shallow convection zones through G-K-early-M stars with gradually deeper convection zones, and they end with the fully convective M dwarf stars, depicting the change of the dynamo type with the internal differences of the main sequence stars in connection with the FIP-bias values.

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