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Table 3:

Reference results for the parameters of the radial p modes.
$\ell$ $\nu_{n,\ell}$ ($\mu $Hz) agr.( $\nu_{n,\ell}$) H0,n (ppm$^2/\mu$Hz) agr.(H0,n) $\Gamma_n$ ($\mu $Hz) agr.($\Gamma_n$) an (ppm) agr.(an) $H_{\ell,n}/B(\nu_{n,\ell})$
0 $ 799.70\pm 0.27$ $\bullet$ $2.55^{\rm +0.80}_{-0.61}$ $\bullet$ $1.58^{\rm +0.42}_{-0.33}$ $\bullet$ $3.55^{\rm +0.67}_{-0.56}$ $\bullet$ 2.23
0 $ 855.30\pm 0.73$ $\bullet$ $2.10^{\rm +0.59}_{-0.46}$ $\bullet$ $2.97^{\rm +0.72}_{-0.58}$ $\bullet$ $4.42^{\rm +0.77}_{-0.65}$ $\bullet$ 1.94
0 $ 909.92\pm 0.26$ $\bullet$ $3.13^{\rm +0.82}_{-0.65}$ $\bullet$ $2.00^{\rm +0.43}_{-0.35}$ $\bullet$ $4.44^{\rm +0.70}_{-0.60}$ $\bullet$ 3.03
0 $ 965.16\pm 0.36$ $\bullet$ $4.05^{\rm +0.96}_{-0.78}$ $\bullet$ $2.37^{\rm +0.43}_{-0.37}$ $\bullet$ $5.49^{\rm +0.83}_{-0.72}$ $\bullet$ 4.09
0 $1021.81\pm 0.28$ $\bullet$ $4.56^{\rm +1.15}_{-0.92}$ $\bullet$ $2.03^{\rm +0.41}_{-0.34}$ $\bullet$ $5.40^{\rm +0.80}_{-0.70}$ $\bullet$ 4.78
0 $1078.97\pm 0.33$ $\bullet$ $4.77^{\rm +1.10}_{-0.90}$ $\bullet$ $2.08^{\rm +0.35}_{-0.30}$ $\bullet$ $5.58^{\rm +0.80}_{-0.70}$ $\bullet$ 5.18
0 $1135.32\pm 0.34$ $\bullet$ $3.49^{\rm +0.83}_{-0.67}$ $\bullet$ $2.37^{\rm +0.44}_{-0.37}$ $\bullet$ $5.09^{\rm +0.86}_{-0.73}$ $\bullet$ 3.90
0 $1192.12\pm 0.45$ $\bullet$ $2.29^{\rm +0.67}_{-0.52}$ $\bullet$ $2.51^{\rm +0.68}_{-0.53}$ $1.8~\sigma$ $4.25^{\rm +0.80}_{-0.67}$ $\bullet$ 2.63
0 $1250.12\pm 0.89$ $\bullet$ $1.15^{\rm +0.32}_{-0.25}$ $\bullet$ $3.90^{\rm +1.00}_{-0.80}$ $\bullet$ $3.76^{\rm +4.04}_{-1.95}$ $\bullet$ 1.36

Notes. The heights given here are those of the $\ell =0$ modes (the heights of non-radial modes are computed using height ratios, see Sect. 5.3.1). The agreement (agr.) between the teams is given for each fitted parameter. Filled circles indicate that at least four of the five teams agreed on the value within 1 $\sigma $. $X~\sigma$ indicates that more than one team disagrees with the value, and that the five teams agree within $X~\sigma$ (X>1).


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