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Table A.1

Comparison of the ToF5 and accelerated CMS results for two representative models.

Method J2 × 106 J4 × 106 J6 × 106 J8 × 106 J10 × 106 Z1 Z2 Mcore (M)
Error bar(a) 0.028 0.037 0.087 0.205 0.420
ΔJ2i(b) 50.54 7.5883 4.0932 −5.5055 3.6600
ΔJ2i(c) −3.855 3.032 2.187 −5.023 3.399

A ToF5-fit 16273.43 −946.7607 84.02621 −9.35601 1.20546 0.0640 0.0247 14.89
B CMS 16297.04 −947.9340 84.12987 −9.38624 1.20849
A-B −23.61 1.1733 −0.10366 0.03023 −0.00303
C CMS-fit 16273.47 −946.7624 84.03046 −9.37464 1.20687 0.0639 0.0221 15.01
A-C Offsets −0.04 0.0017 −0.00425 0.01863 −0.00141 0.0001 0.0026 −0.12

D ToF5-fit 16273.47 −946.7622 84.63584 −9.48500 1.22661 0.0508 0.0404 13.28
E CMS 16293.55 −947.7614 84.72266 −9.51365 1.22936
D-E −20.08 0.9992 −0.08682 0.02865 −0.00275
F CMS-fit 16273.44 −946.7483 84.63424 −9.50304 1.22785 0.0507 0.0383 13.38
D-F Offsets 0.03 −0.0139 0.00160 0.01804 −0.00124 0.0001 0.0021 −0.10

Notes. The top panel shows the uncertainties on Saturn’s gravity harmonics. The second panel (A-C) displays the predictions of the interior model using REOS3b. The bottom panel (D-F) displays the predictions of the interior model using MH13+SCvH. (a) Error bars of the Cassini Grand Finale gravity measurements from Iess et al. (2019). (b) Flow-induced gravity corrections of Galanti et al. (2019). (c)Flow-induced gravity corrections of Kong et al. (2019).

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