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Table 2

Orbital and physical parameters of TOI-5795 b.

Parameter Unit Value
Light curve parameters
Porb day 6.1406325 ± 0.0000054
T0 BJDTDB 2459770.673970.00061+0.00060$2\,459\,770.67397_{-0.00061}^{+0.00060}$
T14 hr 3.4070.026+0.028$3.407^{+0.028}_{-0.026}$
Rp/R* 0.0477±0.0006
b 0.290.14+0.12$0.29^{+0.12}_{-0.14}$
i deg 88.540.55+0.68$88.54^{+0.68}_{-0.55}$
a/R* 12.650.35+0.34$12.65^{+0.34}_{-0.35}$
Limb-darkening coefficients(a)
q1, TESS 0.200.08+0.15$0.20^{+0.15}_{-0.08}$
q2, TESS 0.410.24+0.33$0.41^{+0.33}_{-0.24}$
q1, B 0.420.29+0.36$0.42^{+0.36}_{-0.29}$
q2, B 0.520.29+0.31$0.52^{+0.31}_{-0.29}$
q1, LCO 0.500.32+0.33$0.50^{+0.33}_{-0.32}$
q2, LCO 0.540.33+0.32$0.54^{+0.32}_{-0.33}$
RV parameters
K m s−1 8.971.74+1.51$8.97^{+1.51}_{-1.74}$
esinω$\sqrt{e}\sin\omega$ 0.1970.105+0.101$0.197^{+0.101}_{-0.105}$
ecosω$\sqrt{e}\cos\omega$ 0.3170.142+0.107$0.317^{+0.107}_{-0.142}$
e(b) <0.25
ω deg 31.6717.83+25.07$31.67^{+25.07}_{-17.83}$
RV jitter HARPS m s−1 3.751.08+1.23$3.75^{+1.23}_{-1.08}$
Derived
Mp M 23.664.61+4.09$23.66^{+4.09}_{-4.61}$
Rp R 5.62 ±0.11
ρp g cm−3 0.73 ± 0.13
log gp cgs 7.33 ± 1.29
a au 0.064 ±0.002
Teq(c)$T_{\rm eq}^{(c)}$ K 1136.7818.02+18.89$1136.78^{+18.89}_{-18.02}$
TSM(d) 10315+25$103^{+25}_{-15}$
GP coefficients
σGP 0.00160 ± 0.00014
ρGP 0.98 ± 0.09

Notes. The median values of the best-fit parameters for TOI-5795 b, along with their upper and lower 68% credibility intervals as uncertainties. These values, both fitted and derived, were obtained from the posterior distributions of the corresponding models. (a)q1 ≡ (u1 + u2)2 and q2 ≡ 0.5 (u1 + u2)−1, where u1 and u2 are the LD coefficients of the quadratic law (Kipping 2013). (b)The 95% (2σ) confidence upper limit on the eccentricity determined when √e cos ω and √e sin ω are allowed to vary in the fit. (c)This represents the equilibrium temperature assuming a Bond albedo of zero and an uniform redistribution of heat to the night side. (d)Transmission spectroscopy metric (TSM; Kempton et al. 2018).

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