Table 5
Fourier and photodynamical mass estimates.
| Parameter | Units | Median and 68.3% CI | MAP | vR/vS, AS (1) | Petigura(2) | From Radii(3) |
|---|---|---|---|---|---|---|
| Photodyn | Photodyn | Fourier | Photodyn | |||
| 10 yr | 10 yr | 10 yr | 3.3 yr | |||
| mb | M⊕ | 30.8 ± 1.3 | 29.62 | 30.03 | 32.4 ± 1.7 | 39.6 |
| mc | M⊕ | 11.12 ± 0.44 | 10.94 | 11.08 | 10.8 ± 0.6 | 18.0 |
| Δmb,c/mb,c | −0.04, −0.02 | −0.02, −0.004 | +0.05, +0.03 | +0.29, +0.62 | ||
| ρb | g cm−3 | 0.59 | 0.57 | 0.58 | 0.52 | 0.76 |
| ρc | g cm−3 | 1.05 | 1.03 | 1.04 | 0.86 | 1.69 |
![]() |
d | 2711.2 | (2751.9) | |||
| PR | d | 717.4 | ||||
![]() |
min | 53.4, (41.7) | ||||
![]() |
min | 233.2, (148.3) | ||||
| βS, βR | deg | ![]() |
[−103.9], [−41.9] | (−103.5, −35.7) | ||
| λn | deg | ![]() |
82.8 | 37.5(4) | ||
| R | ![]() |
[15.49] | 13.28 | [15.7] | ||
| ∆σ | ![]() |
[0.0029] | 0.0030 | [0.0029] | ||
![]() |
![]() |
[0.015] (0.069) | 0.015 | ![]() |
||
![]() |
![]() |
[0.045] (0.078) | 0.043 | ![]() |
Notes. (1): νR/νS, AS / Fourier A uses the frequency ratio and superamplitudes only to estimate masses; (2): Petigura / Photodyn uses system parameters from the photodynamical analysis of Petigura et al. (2020); (3): Estimates using mass-radius relation mp/ME = (Rp/0.56 RE)1/0.67 (Müller et al. 2024); (4): Petigura et al. (2020) value minus 180° to account for the fact that the authors assumed Ωb(tref) = 0; [Square brackets] show the quantity calculated analytically from elements and masses using the formalism of Mardling (2025a); ∆mb,c/mb,c = relative difference in masses compared to median value;
(defined from ephemeris periods such that
) listed in the last column for comparison with the Fourier superperiod; Boldface entries: highlighted for comparison; Amplitudes and phases in brackets were not used directly in mass estimates. Last two rows: Entries in brackets are the median and 68.3% CI eccentricities for comparison with the fixed-point values
and
. The reference mean densities are ρSaturn = 0.69 g cm−3, ρUranus = 1.15 g cm−3.
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