Table 9:

Global parameter posterior estimates for HD 49933. i represents the inclination angle of the star. $\nu _{\rm s}$ is the rotational splitting, Vl=1 and Vl=2 the relative height of l=1 and l=2 modes, respectively. $\Delta \nu $ represent the large separation.

Model
$M^1_{\rm A}$ $M^1_{\rm B}$

Probability
62.8% 0.2%
i $(^\circ$) median 52 23
$1 \sigma_+/1 \sigma_- $ $8\hspace{0.5mm}/\hspace{0.5mm}8$ $17\hspace{0.5mm}/\hspace{0.5mm}15$
  $2 \sigma_+$/ $2 \sigma_-$ $20\hspace{0.5mm}/\hspace{0.5mm}18$ $36\hspace{0.5mm}/\hspace{0.5mm}22$
$\nu _{\rm s}$ ( $\mu {\rm Hz}$) median 3.20 3.34
$1 \sigma_+/1 \sigma_- $ $0.28\hspace{0.5mm}/\hspace{0.5mm}0.26$ $0.34\hspace{0.5mm}/\hspace{0.5mm}0.35$
  $2 \sigma_+/2 \sigma_- $ $0.59\hspace{0.5mm}/\hspace{0.5mm}0.54$ $0.69\hspace{0.5mm}/\hspace{0.5mm}0.69$
Vl=1 median 1.00 0.93
$1 \sigma_+/1 \sigma_- $ $0.09\hspace{0.5mm}/\hspace{0.5mm}0.09$ $0.08\hspace{0.5mm}/\hspace{0.5mm}0.09$
  $2 \sigma_+/ 2 \sigma$ $0.20\hspace{0.5mm}/\hspace{0.5mm}0.17$ $0.19\hspace{0.5mm}/\hspace{0.5mm}0.15$
$\Delta \nu $ ( $\mu {\rm Hz}$) median 86.04 86.04
$1 \sigma_+/1 \sigma_- $ $0.13\hspace{0.5mm}/\hspace{0.5mm}0.14$ $0.14\hspace{0.5mm}/\hspace{0.5mm}0.16$
  $2 \sigma_+/2 \sigma_- $ $0.28\hspace{0.5mm}/\hspace{0.5mm}0.33$ $0.28\hspace{0.5mm}/\hspace{0.5mm}0.33$

Model
$M^2_{\rm A}$ $M^2_{\rm B}$

Probability
14% 23%
i $(^\circ$) median 50 28
$1 \sigma_+/1 \sigma_- $ $8\hspace{0.5mm}/\hspace{0.5mm}7$ $19\hspace{0.5mm}/\hspace{0.5mm}17$
  $2 \sigma_+$/ $2 \sigma_-$ $15\hspace{0.5mm}/\hspace{0.5mm}21$ $39\hspace{0.5mm}/\hspace{0.5mm}27$
$\nu _{\rm s}$ ( $\mu {\rm Hz}$) median 3.17 3.37
$1 \sigma_+/1 \sigma_- $ $0.27\hspace{0.5mm}/\hspace{0.5mm}0.25$ $0.32\hspace{0.5mm}/\hspace{0.5mm}0.35$
  $2 \sigma_+/2 \sigma_- $ $0.57\hspace{0.5mm}/\hspace{0.5mm}0.52$ $0.68\hspace{0.5mm}/\hspace{0.5mm}0.70$
Vl=1 median 1.11 1.22
$1 \sigma_+/1 \sigma_- $ $0.16\hspace{0.5mm}/\hspace{0.5mm}0.11$ $0.22\hspace{0.5mm}/\hspace{0.5mm}0.16$
  $2 \sigma_+/ 2 \sigma$ $0.36\hspace{0.5mm}/\hspace{0.5mm}0.21$ $0.52\hspace{0.5mm}/\hspace{0.5mm}0.28$
Vl=2 median 0.13 0.35
$1 \sigma_+/1 \sigma_- $ $0.14\hspace{0.5mm}/\hspace{0.5mm}0.09$ $0.21\hspace{0.5mm}/\hspace{0.5mm}0.15$
  $2 \sigma_+/2 \sigma_- $ $0.34\hspace{0.5mm}/\hspace{0.5mm}0.13$ $0.50\hspace{0.5mm}/\hspace{0.5mm}0.27$
$\Delta \nu $ ( $\mu {\rm Hz}$) median 86.05 86.00
$1 \sigma_+/1 \sigma_- $ $0.13\hspace{0.5mm}/\hspace{0.5mm}0.15$ $0.16\hspace{0.5mm}/\hspace{0.5mm}0.19$
  $2 \sigma_+/2 \sigma_- $ $0.30\hspace{0.5mm}/\hspace{0.5mm}0.42$ $0.32\hspace{0.5mm}/\hspace{0.5mm}0.42$
i represents the inclination angle of the star. $\nu _{\rm s}$ is the rotational splitting, Vl=1 and Vl=2 the relative height of l=1 and l=2 modes, respectively. $\Delta \nu $ represent the large separation.

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