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Table 1.

RHD simulation parameters.

Simulation M L R Teff logg tavg Ppuls σpuls P σP Px Py
M L AU K (cgs) yr yr yr AU AU AU AU
st26gm07n002 1.0 6986 2.04 2524 –0.85 25.35 1.625 0.307 0.262 0.187 –0.100 0.046
st26gm07n001 1.0 6953 1.87 2635 –0.77 27.74 1.416 0.256 0.275 0.198 –0.098 0.024
st28gm06n26 1.0 6955 1.73 2737 –0.70 25.35 1.290 0.317 0.241 0.152 –0.068 –0.002
st29gm06n001 1.0 6948 1.62 2822 –0.65 25.35 1.150 0.314 0.266 0.174 –0.098 0.016
st27gm06n001 1.0 4982 1.61 2610 –0.64 28.53 1.230 0.088 0.150 0.101 –0.027 0.027
st28gm05n002 1.0 4978 1.46 2742 –0.56 25.35 1.077 0.104 0.133 0.077 –0.002 0.033
st28gm05n001 1.0 4990 1.40 2798 –0.52 25.36 1.026 0.135 0.183 0.131 –0.057 0.0174
st29gm04n001 1.0 4982 1.37 2827 –0.50 25.35 0.927 0.100 0.152 0.078 –0.002 0.023

Notes. The table shows the simulation name, the mass M, the average emitted luminosity L, the average approximate stellar radius R (we note that the radii vary by about 20% during one pulsation period), effective temperature Teff, surface gravity logg, the pulsation period Ppuls, the half of the distribution of the pulsation frequencies σpuls, and the stellar time tavg used for the averaging of the rest of the quantities. All these quantities are from Freytag et al. (2017). The last four columns are the time-averaged value of the photocentre displacement ⟨P⟩=⟨(Px2 + Py2)(1/2)⟩, its standard deviation (σP), and the time-average of Px and Py.

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