Table 2.

Best-fitting parameters for three our solutions and two solutions in Barnes et al. (2013).*

ParameterShort solutionMiddle solutionLong solutionB13 (Ms = 0.34 M) B13 (Ms = 0.44 M)
ρs (g cm−3)0.32 ± 0.010.27 ± 0.010.30 ± 0.010.43 ± 0.010.57 ± 0.02
P  s (d)0.390 ± 0.0080.367 ± 0.0060.331 ± 0.0080.4484100.448413
i  s (°)123.9 ± 2.2128.2 ± 1.7131.3 ± 1.5119.4 ± 0.3120.3 ± 1.3
M  p/Ms0.0129 ± 0.00140.0178 ± 0.00090.0199 ± 0.00080.0084 ± 0.00060.0078 ± 0.0007
R  p/Rs0.169 ± 0.0030.208 ± 0.0080.289 ± 0.0160.159 ± 0.0070.164 ± 0.007
i  orb (°)62.9 ± 0.855.3 ± 0.550.9 ± 0.665.2 ± 1.669.3 ± 1.3
Ω (°)133.4 ± 3.3131.2 ± 2.4130.2 ± 2.2136.1 ± 5.2125.5 ± 0.5
ϕ (°)75.3 ± 2.585.8 ± 1.892.3 ± 1.669 ± 373.1 ± 0.6
|$P_{\dot{\Omega }}$| (d)198.7 ± 15.6474.6 ± 21.1826.9 ± 53.3292.6581.2
ParameterShort solutionMiddle solutionLong solutionB13 (Ms = 0.34 M) B13 (Ms = 0.44 M)
ρs (g cm−3)0.32 ± 0.010.27 ± 0.010.30 ± 0.010.43 ± 0.010.57 ± 0.02
P  s (d)0.390 ± 0.0080.367 ± 0.0060.331 ± 0.0080.4484100.448413
i  s (°)123.9 ± 2.2128.2 ± 1.7131.3 ± 1.5119.4 ± 0.3120.3 ± 1.3
M  p/Ms0.0129 ± 0.00140.0178 ± 0.00090.0199 ± 0.00080.0084 ± 0.00060.0078 ± 0.0007
R  p/Rs0.169 ± 0.0030.208 ± 0.0080.289 ± 0.0160.159 ± 0.0070.164 ± 0.007
i  orb (°)62.9 ± 0.855.3 ± 0.550.9 ± 0.665.2 ± 1.669.3 ± 1.3
Ω (°)133.4 ± 3.3131.2 ± 2.4130.2 ± 2.2136.1 ± 5.2125.5 ± 0.5
ϕ (°)75.3 ± 2.585.8 ± 1.892.3 ± 1.669 ± 373.1 ± 0.6
|$P_{\dot{\Omega }}$| (d)198.7 ± 15.6474.6 ± 21.1826.9 ± 53.3292.6581.2

*Our angular parameters (is, iorb, Ω) are evaluated at tc = 2455543.9402 HJD (Heliocentric Julian Date) while those of B13 are at tc = 2455536.7680 HJD, the interval of which corresponds to 7.1722 d or 16 transits. Spin–orbit angle ϕ is time-invariant.

Table 2.

Best-fitting parameters for three our solutions and two solutions in Barnes et al. (2013).*

ParameterShort solutionMiddle solutionLong solutionB13 (Ms = 0.34 M) B13 (Ms = 0.44 M)
ρs (g cm−3)0.32 ± 0.010.27 ± 0.010.30 ± 0.010.43 ± 0.010.57 ± 0.02
P  s (d)0.390 ± 0.0080.367 ± 0.0060.331 ± 0.0080.4484100.448413
i  s (°)123.9 ± 2.2128.2 ± 1.7131.3 ± 1.5119.4 ± 0.3120.3 ± 1.3
M  p/Ms0.0129 ± 0.00140.0178 ± 0.00090.0199 ± 0.00080.0084 ± 0.00060.0078 ± 0.0007
R  p/Rs0.169 ± 0.0030.208 ± 0.0080.289 ± 0.0160.159 ± 0.0070.164 ± 0.007
i  orb (°)62.9 ± 0.855.3 ± 0.550.9 ± 0.665.2 ± 1.669.3 ± 1.3
Ω (°)133.4 ± 3.3131.2 ± 2.4130.2 ± 2.2136.1 ± 5.2125.5 ± 0.5
ϕ (°)75.3 ± 2.585.8 ± 1.892.3 ± 1.669 ± 373.1 ± 0.6
|$P_{\dot{\Omega }}$| (d)198.7 ± 15.6474.6 ± 21.1826.9 ± 53.3292.6581.2
ParameterShort solutionMiddle solutionLong solutionB13 (Ms = 0.34 M) B13 (Ms = 0.44 M)
ρs (g cm−3)0.32 ± 0.010.27 ± 0.010.30 ± 0.010.43 ± 0.010.57 ± 0.02
P  s (d)0.390 ± 0.0080.367 ± 0.0060.331 ± 0.0080.4484100.448413
i  s (°)123.9 ± 2.2128.2 ± 1.7131.3 ± 1.5119.4 ± 0.3120.3 ± 1.3
M  p/Ms0.0129 ± 0.00140.0178 ± 0.00090.0199 ± 0.00080.0084 ± 0.00060.0078 ± 0.0007
R  p/Rs0.169 ± 0.0030.208 ± 0.0080.289 ± 0.0160.159 ± 0.0070.164 ± 0.007
i  orb (°)62.9 ± 0.855.3 ± 0.550.9 ± 0.665.2 ± 1.669.3 ± 1.3
Ω (°)133.4 ± 3.3131.2 ± 2.4130.2 ± 2.2136.1 ± 5.2125.5 ± 0.5
ϕ (°)75.3 ± 2.585.8 ± 1.892.3 ± 1.669 ± 373.1 ± 0.6
|$P_{\dot{\Omega }}$| (d)198.7 ± 15.6474.6 ± 21.1826.9 ± 53.3292.6581.2

*Our angular parameters (is, iorb, Ω) are evaluated at tc = 2455543.9402 HJD (Heliocentric Julian Date) while those of B13 are at tc = 2455536.7680 HJD, the interval of which corresponds to 7.1722 d or 16 transits. Spin–orbit angle ϕ is time-invariant.

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