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Table 6

Parameters and coefficients for the phoebe best-fit model to the Kepler light curve for Quarters 012 long cadence data for the non-beaming and beaming cases.

Parameter Non-beaming Beaming

Mass ratio, q 0.199 ± 0.001 0.20 ± 0.03
Secondary mass (M), M2 0.30 ± 0.01 0.29 ± 0.03
Semi-major axis (R), a 106.1 ± 0.5 105.6 ±  0.9
Orbital eccentricity, e 0.71 ± 0.01 0.71 ± 0.02
Argument of periastron (rad), ω 4.0 ± 0.1 4.01 ± 0.06
Orbital inclination (°), i 62 ± 4 61 ± 6
Primary potential, Ω1 16.7 ± 0.2 16.2 ± 0.2
Gamma velocity (km s-1), γ –14.01 ± 0.01 –14.43 ± 0.08
Primary log g (cgs), log g1 3.078  ± 0.007 3.022 ± 0.007
Gravity darkening exponent, GRD 1.00 ± 0.03 1.07 ± 0.03
Primary fractional point radius 0.0644 0.0679
Primary fractional pole radius 0.0637 0.0676
Phase of periastron 0.0121 0.0094
Primary x1 coeff. 0.718 0.717
Primary y1 coeff. 0.716 0.714

Fixed Parameters Values: both Cases

Primary Teff (K) 5000 ± 250
Third light 0.0
Orbital period (d) 94.812 ± 0.002
Time of primary minimum (BJD) 245 019.221 ± 0.008
Primary bolometric albedo 0.6

Notes. The secondary component’s potential, radius and log g are not noted as these parameters have no signature in the light curve and radial velocity data. The fractional radii quoted are the radii relative to the semi-major axis. For the mass and radius of the primary component, see Table 1. The limb darkening coefficients (x1 and y1) are for the square root limb darkening law and were taken from the phoebe limb darkening tables (Prša et al. 2011). For the beaming case we assumed 100% of the flux comes from the primary component.

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