Notes. The table lists the prior, the posterior median, and the 68.3% CI for the photodynamical analysis (Sect. 4.2). The Jacobi orbital elements are given for the reference time t_ref = 2 456 829.222 BJD_TDB.^† Upper limit at 99% confidence. The planetary equilibrium temperature is computed for zero albedo and full day-night heat redistribution. P′ and T′₀ should not be confused with the period or the time of conjunction, respectively, and they were only used to reduce the correlations between jump parameters, replacing the semimajor axis and the mean anomaly at t_ref. ${T^{\prime }}_0\equiv t_{\text{ref}}-\frac{P^{\prime }}{2\pi }\left(M_0-E+e\sin E\right)$ with $E=2\arctan \left\{\sqrt{\frac{1-e}{1+e}\tan \left[\frac{1}{2}\left(\frac{\pi }{2}-\omega \right)\right]}\right\},P^{\prime }\equiv \sqrt{\frac{4{\pi }^2{a}^3}{G{m}_{★}}},K^{\prime }\equiv \frac{m_p\sin i}{m_{★}^{2/3}\sqrt{1+e^2}}{\left(\frac{2\pi G}{P^{\prime }}\right)}^{1/3}$. CODATA 2018: 𝒢 = 6.67430 ×10⁻¹¹m³ kg⁻¹ s⁻². IAU 2012: au = 149 597 870 700 m. IAU 2015: $R_{\odot }^{\text{N}}=6.957\times {10}^8\text{\hspace{0.17em}m,\hspace{0.17em}}{\left(GM\right)}_{\odot }^{\text{N}}=1.3271244\times {10}^{20}{\text{m}}^3{\text{s}}^{-2}$, $R_{e\text{E}}^{\text{N}}=6.3781\times {10}^6\text{\hspace{0.17em}m,\hspace{0.17em}}{\left(GM\right)}_{\text{E}}^{\text{N}}=3.986004\times {10}^{14}{\text{m}}^3{\text{s}}^{-2},M_{\odot }={\left(GM\right)}_{\odot }^{\text{N}}/G,{\text{ME}}_{}={\left(GM\right)}_{\text{E}}^{\text{N}}/G,k^2={\left(GM\right)}_{\odot }^{\text{N}}{\left(86400\text{\hspace{0.17em}s}\right)}^2/{\text{au}}^3$. N(µ, σ): Normal distribution with mean µ and standard deviation σ. U(a, b): A uniform distribution defined between a lower a and upper b limit. S (a, b): A sinusoidal distribution defined between a lower a and upper b limit. Transits occur when the sum of the true anomaly and the argument of pericenter equals −90°.