Properties of stars hosting exoplanets
(A. Brucalassi, G. Casali, L. Magrini, M. Rainer, G. Sacco, N. Sanna, M. Tsantaki)
The recent success of
ground-based and space transit searches (more than 4000 planets have been
detected showing an incredible diversity- http://exoplanet.eu/ ) has ushered exoplanet
research into an era of characterization studies with the goal to
investigate the nature, formation, and evolutionary history of the detected
objects. Transiting planets provide us one of the best ways for characterising
their atmospheres. Our research group in
Arcetri is part of the Ariel project.
Ariel, the Atmospheric Remote-sensing Infrared
Exoplanet Large-survey, has been
selected as the fourth medium-class mission in the ESA Cosmic Vision programme.
During its 4-year mission, Ariel
will study what exoplanets are made of, how they formed and how they evolve, by
surveying a diverse sample of about 1000 extrasolar planets, simultaneously in
visible and infrared wavelengths. It is the first mission dedicated to
measuring the chemical composition and thermal structures of hundreds of
transiting exoplanets. Key factor for the achievement of the scientific goal of
Ariel is the selection
strategy for the definition of the input target list,
that is based on the accurate knowledge of the stellar properties.
Another
important point is that information on the host star composition could provide
stronger constraints on the planet formation region and their migration
mechanisms (Madhusudhan et al. 2016, Turrini et al. 2018).
Finally,
an increasing number of studies have pointed towards the existence of
correlations between the properties and
frequency of the newfound planets and those of their host stars.
In
this context, the correlation
between the stellar metallicity and the frequency of giant planets (Santos et
al, 2004; Valenti & Fischer 2005), the
connection between radius vs. metallicity (Buchhave et al., 2014; Schlaufman
2015), eccentricity vs. metallicity
(Adibekyan et al, 2013), the role of the
abundances of other elements in the host stars are only few examples of
different results that are taking a clear shape as the new planet discoveries
increase, shading light on many details still missing concerning planet
formation and evolution. Such works rely upon
homogeneously and precisely derived stellar parameters.
Our research group is
focused on the derivation of stellar parameters for
the Ariel Reference Target Sample. In addition, it is involved with other
working groups in the calculation of stellar abundances of the same sample. So far, we have conducted a
benchmarking analysis between three different spectroscopic techniques (SweetCat (Santos et al.
2013) - FAMA (Magrini et al. 2016) - FASMA (Tsantaki et al. 2018)) used to determine stellar parameters for a
number of selected targets belonging to the Ariel
reference sample. Moreover, external comparison to
evaluate the results of the different methods used
(Brucalassi et al. 2020, in prep.) have been produced (see Figure 1).
A well-defined target selection strategy and the
definition of the input target list have a fundamental role for maximising the
scientific yield and the achievement of scientific goals of Ariel. This requires an accurate
study of the stellar properties that need to be derived in advance and
continuously updated as the mission approaches
the launch and the target list evolves with the new
exoplanet discoveries.
Figure 1: (From Brucalassi et al.
2020): Comparison of stellar
parameters derived by different methods: Sweet-Cat
vs FAMA (blue) and FASMA (red) for effective temperature (Teff), surface
gravity (log g), metallicity [Fe/H]). The horizontal line is the zero point level. In the parameter space close to Solar
values the agreement among the three methods is good. However, at low and high
temperatures some methods tend to under/overestimate the surface gravity log g.
Right bottom panel: Kiel diagram (log g vs Teff)
using values listed in Sweet-Cat, obtained by FAMA, FASMA and derived by Gaia.
Over-plotted PARSEC isochrones. The outermost tracks correspond to log(age/yr )= 8.95 (bottom track)
and 10.15 (upper track) with [M/H]= 0.058, Z= 0.0198, Y=0.273.
References:
Adibekyan,
V.Z., Figueira, P., Santos, N.C. et al. A&A, 560, A51 (2013).
Brucalassi,
A., Tsantaki, M., Magrini, L. et al. Experimental
Astronomy (2020), in prep.
Magrini,
L., Randich, S., Friel, E., Spina, L. et al. A&A, 558,
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Madhusudhan,
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Santos,
N.C., Sousa, S.G., Mortier, A. et al. A&A, 556, A150 (2013).
Schlaufman,
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