J/AJ/155/177   Obliquities of planetary & eclipsing binary systems  (Dai+, 2018)

Stellar obliquity and magnetic activity of planet-hosting stars and eclipsing binaries based on transit chord correlation. Dai F., Winn J.N., Berta-Thompson Z., Sanchis-Ojeda R., Albrecht S. <Astron. J., 155, 177-177 (2018)> =2018AJ....155..177D 2018AJ....155..177D (SIMBAD/NED BibCode)
ADC_Keywords: Exoplanets ; Binaries, eclipsing ; Stars, masses ; Stars, diameters ; Effective temperatures Keywords: binaries: eclipsing - planetary systems - planets and satellites: general - stars: activity - stars: rotation - starspots Abstract: The light curve of an eclipsing system shows anomalies whenever the eclipsing body passes in front of active regions on the eclipsed star. In some cases, the pattern of anomalies can be used to determine the obliquity Ψ of the eclipsed star. Here we present a method for detecting and analyzing these patterns, based on a statistical test for correlations between the anomalies observed in a sequence of eclipses. Compared to previous methods, ours makes fewer assumptions and is easier to automate. We apply it to a sample of 64 stars with transiting planets and 24 eclipsing binaries for which precise space-based data are available, and for which there was either some indication of flux anomalies or a previously reported obliquity measurement. We were able to determine obliquities for 10 stars with hot Jupiters. In particular we found Ψ~<10° for Kepler-45, which is only the second M dwarf with a measured obliquity. The other eight cases are G and K stars with low obliquities. Among the eclipsing binaries, we were able to determine obliquities in eight cases, all of which are consistent with zero. Our results also reveal some common patterns of stellar activity for magnetically active G and K stars, including persistently active longitudes. Description: The motivation for our work was to develop a more objective method for measuring obliquities that does not rely on explicit spot modeling and can be more easily applied to a large sample of systems. Instead of assuming that the active regions are discrete dark and bright spots, we treat the transit light curve as a measure of the intensity distribution of the stellar photosphere along the transit chord. For convenience, we call this the transit chord correlation (TCC) method, although we do not claim it is a completely new concept. It is closely related to eclipse mapping (Horne 1985MNRAS.213..129H 1985MNRAS.213..129H), which has long been used to probe the brightness distribution of stars and accretion disks. In this paper, we explain the TCC method, validate it through application to systems for which the stellar obliquity has been measured by independent methods, and apply it to all the transiting planets for which the method is currently feasible. We also apply the TCC method to a sample of eclipsing binaries drawn from the Kepler survey. We tried to assemble a collection of all the transit data sets for which there seemed to be a reasonable chance of success for the TCC method. The requirement for high S/N and a large number of consecutive transits restricts us to data from the space missions CoRoT, Kepler, and K2. Tables 1 and 2 summarize the results for the transiting planets and eclipsing binaries, respectively. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file table1.dat 325 64 List of planetary systems searched table2.dat 178 24 List of eclipsing binary systems searched -------------------------------------------------------------------------------- See also: V/133 : Kepler Input Catalog (Kepler Mission Team, 2009) J/A+A/479/865 : CoRoT exoplanet candidates (Loeillet+, 2008) J/ApJ/757/18 : Radial velocities for 16 hot Jupiter host stars (Albrecht+, 2012) J/MNRAS/443/2391 : Light curves of Qatar-2 transit events (Mancini+, 2014) J/AJ/151/68 : Kepler Mission. VII. Eclipsing binaries in DR3 (Kirk+, 2016) J/ApJ/824/15 : Orbital circularization of Kepler eclipsing bin. (Van Eylen+, 2016) J/AJ/154/105 : Parameters of 529 Kepler eclipsing binaries (Kjurkchieva+, 2017) http://exofop.ipac.caltech.edu : The Exoplanet Follow-up Observing Program (ExoFOP) website Byte-by-byte Description of file: table1.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 11 A11 --- Name Planetary system designation (1) 13 A1 --- n_Name [b] Note on Name (2) 15- 25 A11 --- Status Status of the planet (Confirmed or Brown Dwarf) 27- 40 F14.10 d Per [0.85353/125.63243] Orbital period 42- 53 F12.10 d e_Per [1.87e-08/0.0014]? Uncertainty in Per 55- 62 F8.4 --- a/R* [3.16/155.4] Scaled semimajor axis 64- 69 F6.4 --- e_a/R* [0.0039/3]? Lower limit uncertainty in a/R* 71- 76 F6.4 --- E_a/R* [0.0039/3]? Upper limit uncertainty in a/R* 78 A1 --- l_Mp [<] Limit flag on Mp 79- 87 F9.5 Mjup Mp [0.0149/120]? Planetary mass 89- 95 F7.5 Mjup e_Mp [0.0009/8.8]? Lower limit uncertainty in Mp 97-104 F8.5 Mjup E_Mp [0.0009/14]? Upper limit uncertainty in Mp 106-111 F6.4 Rjup Rp [0.149/1.614] Planetary radius 113-118 F6.4 Rjup e_Rp [0.0054/0.79] Lower limit uncertainty in Rp 120-125 F6.4 Rjup E_Rp [0.0054/0.79] Upper limit uncertainty in Rp 127-131 F5.3 Msun M* [0.59/1.54] Mass of the host star 133-137 F5.3 Msun e_M* [0.01/0.62] Lower limit uncertainty in M* 139-143 F5.3 Msun E_M* [0.01/0.62] Upper limit uncertainty in M* 145-149 F5.3 Rsun R* [0.55/2.02] Radius of the host star 151-155 F5.3 Rsun e_R* [0.018/0.927] Lower limit uncertainty in R* 157-161 F5.3 Rsun E_R* [0.018/0.927] Upper limit uncertainty in R* 163-166 I4 K Teff [3820/8500] Effective temperature of the host star 168-170 I3 K e_Teff [32/400] Uncertainty in Teff 172-177 F6.3 d Pphot [1.245/31.6]? Stellar rotation period measured from rotational modulation in the light curve 179-183 F5.3 d e_Pphot [0.014/3.6]? Uncertainty in Pphot 185-190 F6.2 d Ptcc [0.8/115] Stellar rotation period that gives the strongest transit chord correlation (TCC) 192-195 F4.2 d e_Ptcc [0.1/4] Uncertainty in Ptcc 197-200 F4.1 --- Nsigma [0.7/59.6] Statistical significance of correlation compared to the results of scrambling test Nσ 202-206 F5.2 --- Ptcc/Per [0.13/25.82] Ratio between the stellar rotation and orbital periods 208 A1 --- l_PsiUp [<] Limit flag on PsiUp 209-210 I2 deg PsiUp [4/16]? Upper limit on the true obliquity ΨUpper (G1) 212 A1 --- l_lambda [<] Limit flag on lambda 213-217 F5.1 deg lambda [-52/155]? Obliquity constraint from the literature λlit 219-223 F5.1 deg e_lambda [2/140]? Lower limit uncertainty in lambda 225-228 F4.1 deg E_lambda [2/37]? Upper limit uncertainty in lambda 231-238 A8 --- n_lambda System with prograde obliquity 240-284 A45 --- Ref Reference(s) 286-325 A40 --- Bibcode Bibcode of the reference(s) -------------------------------------------------------------------------------- Note (1): The systems are sorted by the significance of correlation in the residual flux. Note (2): Note as follows: b = Systems whose stellar obliquity was previously reported to be low yet did not show strong transit chord correlation (TCC). These systems are likely magnetically inactive: the host stars are above the Kraft break; the light curve lacks rotational modulation. Alternatively, the high impact parameter of the planet indicates that the transit chord might have missed the active latitude. -------------------------------------------------------------------------------- Byte-by-byte Description of file: table2.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 7 I7 --- KIC [2438502/8230809] Kepler Input Catalog number (Cat. V/133) 9- 31 A23 --- Status Status of the eclipsing binary system 33- 44 F12.9 d Per [2.02558/53.2204218] Orbital period 46- 56 F11.9 d e_Per [1.75e-07/0.0083] Uncertainty in Per 58- 64 F7.4 --- ecosw [-0.0873/0.0155]? Eccentricity constraint from Van Eylen et al. (2016, J/ApJ/824/15) e*cos(ω) 66- 71 F6.4 --- e_ecosw [0.0008/0.0118]? Uncertainty in ecosw 73- 78 F6.3 --- a/R* [1.96/22.96] Scaled semimajor axis 80- 87 F8.6 --- R1/R2 [0.0909/0.416822] Primary to secondary star radius ratio 89- 96 F8.6 --- e_R1/R2 [1e-06/0.00162] Uncertainty in R1/R2 98-102 F5.3 Msun M* [0.526/1.431] Mass of the host star 104-108 F5.3 Msun e_M* [0.03/0.305] Uncertainty in M* 110-114 F5.3 Rsun R* [0.512/6.447] Radius of the host star 116-120 F5.3 Rsun e_R* [0.026/1.781] Uncertainty in R* 122-125 I4 K Teff [4648/6348] Effective temperature of the host star 127-129 I3 K e_Teff [62/296] Uncertainty in Teff 131-136 F6.3 d Pphot [2.47/78]? Stellar rotation period measured from rotational modulation in the light curve 138-142 F5.3 d e_Pphot [0.01/3]? Uncertainty in Pphot 144-146 A3 --- n_Pphot [ELV ] Note on Pphot (1) 148-152 F5.2 d Ptcc [0.6/80.4] Stellar rotation period that gives the strongest transit chord correlation (TCC) 154-157 F4.2 d e_Ptcc [0.1/4] Uncertainty in Ptcc 159-162 F4.1 --- Nsigma [1.9/12.6] Statistical significance of correlation compared to the results of scrambling test Nσ 164-167 F4.2 --- Ptcc/Per [0.16/6.62] Ratio between the stellar rotation and orbital periods 169 A1 --- l_PsiUp [<] Limit flag on PsiUp 170-171 I2 deg PsiUp [3/22]? Upper limit on the true obliquity ΨUpper (G1) 173-178 A6 --- Ref [ExoFOP] Reference -------------------------------------------------------------------------------- Note (1): Note as follows: ELV = Unable to measure Pphot because ellipsoidal light variation dominates the flux variation. -------------------------------------------------------------------------------- Global notes: Note (G1): The upper limit on the true obliquity is only calculated when a low stellar obliquity is detected. -------------------------------------------------------------------------------- History: From electronic version of the journal
(End) Tiphaine Pouvreau [CDS] 19-Nov-2018
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