Kepler Object of Interest Network III. Kepler-82f: A new non-transiting $21 M_\bigoplus$ planet from photodynamical modelling
A&A 628, A108 (2019) Context. The Kepler Object of Interest Network (KOINet) is a multi-site network of telescopes around the globe organised for follow-up observations of transiting planet candidate Kepler objects of interest (KOIs) with large transit timing variations (TTVs). The main goal of...
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Zusammenfassung: | A&A 628, A108 (2019) Context. The Kepler Object of Interest Network (KOINet) is a multi-site
network of telescopes around the globe organised for follow-up observations of
transiting planet candidate Kepler objects of interest (KOIs) with large
transit timing variations (TTVs). The main goal of KOINet is the completion of
their TTV curves as the Kepler telescope stopped observing the original Kepler
field in 2013.
Aims. We ensure a comprehensive characterisation of the investigated systems
by analysing Kepler data combined with new ground-based transit data using a
photodynamical model. This method is applied to the Kepler-82 system leading to
its first dynamic analysis.
Methods. In order to provide a coherent description of all observations
simultaneously, we combine the numerical integration of the gravitational
dynamics of a system over the time span of observations with a transit light
curve model. To explore the model parameter space, this photodynamical model is
coupled with a Markov chain Monte Carlo algorithm.
Results. The Kepler-82b/c system shows sinusoidal TTVs due to their near 2:1
resonance dynamical interaction. An additional chopping effect in the TTVs of
Kepler-82c hints to a further planet near the 3:2 or 3:1 resonance. We
photodynamically analysed Kepler long- and short-cadence data and three new
transit observations obtained by KOINet between 2014 and 2018. Our result
reveals a non-transiting outer planet with a mass of
$m_f=20.9\pm1.0\;M_\bigoplus$ near the 3:2 resonance to the outermost known
planet, Kepler-82c. Furthermore, we determined the densities of planets b and c
to the significantly more precise values $\rho_b=0.98_{-0.14}^{+0.10}\;\text{g
cm}^{-3}$ and $\rho_c=0.494_{-0.077}^{+0.066}\;\text{g cm}^{-3}$. |
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DOI: | 10.48550/arxiv.1907.06534 |