The Stars Kepler Missed: Investigating the Kepler Target Selection Function Using Gaia DR2

The Stars Kepler Missed: Investigating the Kepler Target Selection Function Using Gaia DR2

Draft version January 12, 2021 Typeset using LATEX twocolumn style in AASTeX63 The Stars Kepler Missed: Investigating the Kepler Target Selection Function Using Gaia DR2 Linnea M. Wolniewicz,1 Travis A. Berger,2 and Daniel Huber2 1Department of Astrophysical and Planetary Sciences, University of Colorado, 2000 Colorado Ave, Boulder, CO 80305, USA 2Institute for Astronomy, University of Hawai`i, 2680 Woodlawn Drive, Honolulu, HI 96822, USA (Received January 8, 2021) Submitted to AJ ABSTRACT The Kepler Mission revolutionized exoplanet science and stellar astrophysics by obtaining highly precise photometry of over 200,000 stars over 4 years. A critical piece of information to exploit Kepler data is its selection function, since all targets had to be selected from a sample of half a million stars on the Kepler CCDs using limited information. Here we use Gaia DR2 to reconstruct the Kepler selection function and explore possible biases with respect to evolutionary state, stellar multiplicity, and kinematics. We find that the Kepler target selection is nearly complete for stars brighter than Kp < 14 mag and was effective at selecting main-sequence stars, with the fraction of observed stars decreasing from 95% to 60% between 14 < Kp < 16 mag. We find that the observed fraction for subgiant stars is only 10% lower, confirming that a significant number of subgiants selected for observation were believed to be main-sequence stars. Conversely we find a strong selection bias against low-luminosity red giant stars (R ≈ 3 − 5R , Teff ≈ 5500K), dropping from 90% at Kp = 14 mag to below 30% at Kp = 16 mag, confirming that the target selection was efficient at distinguishing dwarfs from giants. We compare the Gaia Re-normalized Unit Weight Error (RUWE) values of the observed and non-observed main sequence stars and find a difference in elevated (> 1.2) RUWE values at ∼ 5 σ significance, suggesting that the Kepler target selection shows some bias against either close or wide binaries. We furthermore use the Gaia proper motions to show that the Kepler selection function was unbiased with respect to kinematics. 1. INTRODUCTION cucci et al. 2019; Hsu et al. 2019; Zink & Hansen 2019; The Kepler mission (Borucki et al. 2010), officially re- Garrett et al. 2018; Kopparapu et al. 2018; Mulders et al. tired in 2018, has left behind a legacy dataset for stellar 2018; Burke et al. 2015; Foreman-Mackey et al. 2014; astrophysics and exoplanet science. One of the biggest Dong & Zhu 2013; Youdin 2011). A complicating fac- breakthroughs enabled by Kepler was our understanding tor for many of these studies is the presence of stellar of exoplanet occurrence rates as a function of planet size, companions to Kepler targets (Adams et al. 2012; Lillo- orbital period and stellar type. For example, many plan- Box et al. 2012; Dressing et al. 2014; Law et al. 2014; ets observed around Kepler host stars have been found Baranec et al. 2016; Furlan et al. 2017; Ziegler et al. to have sizes between Earth and Neptune (Howard et al. 2018), which can have significant effects on exoplanet 2012), a population that is absent in our own solar sys- demographics both by biasing planet radii (Teske et al. 2018) and through astrophysical effects such as the sup- arXiv:2101.03190v1 [astro-ph.SR] 8 Jan 2021 tem. Dressing & Charbonneau(2013) found that for the M dwarf stars in the Kepler sample, the Earth-sized pression of planet formation (Kraus et al. 2016). In ad- dition to exoplanet demographics, a number of studies (0:5 − 1:4 R⊕) planetary occurrence rate is 0.51 planets per star for orbital periods less than 50 days, signifi- have used asteroseismology of red giants to explore stel- cantly higher than the 0.26 planetary occurrence rate lar populations in the Kepler field (Miglio et al. 2013; found by Petigura et al.(2013) for Earth-sized planets Pinsonneault et al. 2014; Sharma et al. 2016). around solar-type stars with orbital periods between 5- A critical piece of information for Kepler exoplanet 100 days. A large number of studies have since explored and stellar population studies is the process through planet occurrence as a function of orbital period, planet which targets were selected. For example, most planet size and stellar spectral type using the Kepler sample occurrence rates studies have so far assumed that the (Bryson et al. 2020; Kunimoto & Matthews 2020; Pas- Kepler target selection function is unbiased with respect 2 Wolniewicz et al. to stellar multiplicity. However, Kepler was forced to ties and (2) whether the selection of targets was biased select targets, as only 200,000 stars could be observed with respect to stellar multiplicity. Understanding any over the course of the mission. Previous attempts to potential biases in the selection function has important re-create the Kepler target selection method found that implications for exoplanet science and any future deter- binary stars were selected at similar rates as single-star minations of planetary occurrence rates using the Kepler systems and that the MS dwarf population was under- target sample. estimated (Farmer et al. 2013). However, Farmer et al. (2013) re-created the Kepler selection function using a 2. METHODOLOGY synthetic population, and so many of the underlying as- 2.1. Catalog Cross-matching sumptions and biases of the selection function remain We started with a subset of 2.4 million targets within unexplored. the KIC that are located in the Kepler field of view, The basis for the Kepler target selection was the Ke- which we downloaded from the Mikulski Archive for pler Input Catalog (KIC), which contains physical prop- Space Telescopes (MAST) 1. We focus on Kepler stars erties and photometric data for sources in the Kepler with Kp < 16 mag, as nearly all Kepler targets were field of view (Brown et al. 2011). The primary goal of below this threshold (Batalha et al. 2010). the KIC was to distinguish cool dwarf stars from red As a first step, we cross-matched the KIC with Gaia giants, with an expected reliability rate of 98% (Brown DR2 to obtain Gaia information for each star in the et al. 2011). The KIC used broadband photometry to KIC. To do this, we used the Centre de Donn´ees as- infer stellar parameters for all of their stars, however tronomiques de Strasbourg (CDS) cross-match 2. This the log(g) values were imprecise as they were only con- service is provided by the Universit´ede Strasbourg and strained by photometry using the D51 filter. Kepler joins any VizieR data, in this case Gaia DR2, with a pri- selected the optimal targets for observation using the vate data table based on the right ascension (RA) and KIC, with a goal of selecting solar type stars that could declination (Dec) of the stars. host terrestrial-sized planets (Batalha et al. 2010). The We conducted a positional match with a matching ra- highest priority targets were solar-type stars where it dius of 5 arcseconds. Frequently multiple Gaia stars would be possible to detect an Earth-sized planet in the were matched to a single Kepler ID, as the stars were habitable zone (HZ). The next criterion of the selection located at similar RA and Dec. We removed duplicates process was to include stars that were brighter than 14th by selecting only the Kepler and Gaia ID's associated magnitude in the Kepler passband (Kp). The following with the most similar magnitudes in the Kepler pass- highest priority targets were the brightest stars where band Kp and Gaia passband (G). terrestrial-sized planets would be detectable in the HZ, We then extracted Gaia Re-normalized unit weight even if they were as faint as 15 or 16 magnitudes. Fi- error (RUWE) values for all sources. The unit weight nally, the criterion for detectable planets in the HZ was error (UWE) values are a representation of the nor- relaxed, allowing stars that would benefit from addi- malized chi-squared values resulting from the fitting of tional transit data to be observed. This created a list of Gaia DR2 sources to single-star point spread functions 261,363 stars brighter than 16th magnitude in the Ke- (PSFs). The RUWE value corresponds to a PSF fitting pler passband, which was reduced to less than 200,000 corrected for color-dependent biases. RUWE values cen- stars due to mission constraints (Batalha et al. 2010). ter around 1.0, but can be large if the fit is not good The recent Gaia second data release (DR2) now pro- or there is more noise than expected. A large RUWE vides a unique opportunity to look back at the Kepler value, such as 1.2 or higher, indicates a multi-stellar sys- target sample and better understand its selection func- tem where the presence of stellar companions increases tion (Gaia Collaboration et al. 2018). In particular, the noise. RUWE values above 1.2 have been shown to Gaia DR2 has provided high-precision parallaxes for a be indicators of binaries that are closer than the typical total of 1,692,919,135 sources (Lindegren et al. 2018) and ∼1" resolution limits of Gaia (Evans 2018). includes nearly all the stars in the Kepler field of view, including those not observed by Kepler. The Gaia DR2 2.2. Downselection of targets on the Kepler CCDs parallaxes can be used to vastly improve the properties of stars in the Kepler field (Berger et al. 2018). The Kepler telescope required a 90 degree roll about With Gaia DR2 we can now conduct a detailed in- its optical axis every three months { the length of a Ke- vestigation of the Kepler target selection function.

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