Figure 7.
Corner plots for the G102 white light-curve fit using a linear long-term trend (left-hand panel) and a quadratic long-term trend (right-hand panel). In the case of the quadratic trend, clear correlations between some parameters of the systematics model ($n^{\rm for}_{\rm w}$, $n^{\rm rev}_{\rm w}$, and $r_{\rm a2}$) and the planet-to-star ratio (R$_{\rm p}$/R$_{\rm s}$) can be seen, as highlighted by the green and red posteriors. Notably, $r_{\rm a2}$, the additional parameter which is added to the quadratic fitting has strong correlations with $n^{\rm for}_{\rm w}$, $n^{\rm rev}_{\rm w}$. In the linear fit, $n^{\rm for}_{\rm w}$ and $n^{\rm rev}_{\rm w}$ are not correlated with the transit depth.

Corner plots for the G102 white light-curve fit using a linear long-term trend (left-hand panel) and a quadratic long-term trend (right-hand panel). In the case of the quadratic trend, clear correlations between some parameters of the systematics model (⁠|$n^{\rm for}_{\rm w}$|⁠, |$n^{\rm rev}_{\rm w}$|⁠, and |$r_{\rm a2}$|⁠) and the planet-to-star ratio (R|$_{\rm p}$|/R|$_{\rm s}$|⁠) can be seen, as highlighted by the green and red posteriors. Notably, |$r_{\rm a2}$|⁠, the additional parameter which is added to the quadratic fitting has strong correlations with |$n^{\rm for}_{\rm w}$|⁠, |$n^{\rm rev}_{\rm w}$|⁠. In the linear fit, |$n^{\rm for}_{\rm w}$| and |$n^{\rm rev}_{\rm w}$| are not correlated with the transit depth.

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