Table 3
Summary of the results obtained from the Gaussian fits to the detected H I Balmer lines.
Gaussian fit | NLTE model | |||||||
---|---|---|---|---|---|---|---|---|
Line (a) | Depth (%) | Rp | FWHM (km/s) | v (km/s) | ![]() |
vmic (km/s) | vmac (km/s) | ![]() |
Hα | 0.97 ± 0.02 | 1.56 ± 0.01 | 49.25 ± 0.95 | −3.34 ± 0.36 | 1.37 | 2.0 ± 1.5 | 21 ± 3 | 0.66 |
Hβ | 0.64 ± 0.02 | 1.39 ± 0.01 | 45.0 ± 1.58 | −5.67 ± 0.61 | 1.08 | 1.0 ± 0.8 | 24 ± 1 | 0.71 |
Hγ | 0.51 ± 0.03 | 1.33 ± 0.01 | 36.63 ± 2.17 | −5.74 ± 0.86 | 0.66 | 3.0 ± 0.5 | 24 ± 2 | 0.6 |
Hδ | 0.62 ± 0.05 | 1.38 ± 0.03 | 28.97 ± 2.79 | −8.24 ± 1.13 | 1.03 | 1.0 ± 1.2 | 10 ± 12 | 0.9 |
Hϵ | 0.39 ± 0.06 | 1.25 ± 0.03 | 30.65 ± 5.35 | −5.36 ± 2.11 | 0.7 | 1.0 ± 1.7 | 19 ± 16 | 0.83 |
Hζ | 0.92 ± 0.16 | 1.53 ± 0.08 | 26.1 ± 5.4 | −7.56 ± 2.16 | 3.6 | 14.0 ± 4.8 | 1 ± 14 | 3.75 |
Notes. We report the Depth, FWHM, and v columns representing the Gaussian best-fit parameters, while Rp is the transit depth translated into planetary radii. vmic and vmac are the micro- and macro-turbulence velocity, respectively, for the best-fitting NLTE model. For both analyses, we also report the reduced chi-squared, (a)For each line, we show the wavelength in Å.
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