KNOW the STAR, KNOW the PLANET. II. a STELLAR COMPANION to the HOST STAR of the ECCENTRIC EXOPLANET HD 8673B Lewis C

KNOW the STAR, KNOW the PLANET. II. a STELLAR COMPANION to the HOST STAR of the ECCENTRIC EXOPLANET HD 8673B Lewis C

The Astronomical Journal, 149:144 (6pp), 2015 April doi:10.1088/0004-6256/149/4/144 © 2015. The American Astronomical Society. All rights reserved. KNOW THE STAR, KNOW THE PLANET. II. A STELLAR COMPANION TO THE HOST STAR OF THE ECCENTRIC EXOPLANET HD 8673B Lewis C. Roberts, Jr.1, Brian D. Mason2, Christopher R. Neyman3, Yanqin Wu4, Reed L. Riddle5, J. Christopher Shelton1, John Angione1,12, Christoph Baranec6, Antonin Bouchez7,8, Khanh Bui5, Rick Burruss1, Mahesh Burse9, Pravin Chordia9, Ernest Croner5, Hillol Das9, Richard G. Dekany5, Stephen Guiwits10, David Hale5, John Henning5, Shrinivas Kulkarni5, Nicholas Law11, Dan McKenna5, Jennifer Milburn5, Dean Palmer1, Sujit Punnadi9, A. N. Ramaprakash9, Jennifer E. Roberts1, Shriharsh P. Tendulkar5, Thang Trinh1, Mitchell Troy1, Tuan Truong1, and Jeff Zolkower5 1 Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Drive, Pasadena CA 91109, USA; [email protected] 2 U.S. Naval Observatory, 3450 Massachusetts Avenue, NW, Washington, DC 20392-5420, USA 3 W. M. Keck Observatory, California Association for Research in Astronomy, 65-1120 Mamalahoa Hwy, Kamuela, HI 96743, USA 4 Department of Astronomy and Astrophysics, University of Toronto, ON M5S 3H4, Canada 5 Division of Physics, Mathematics, and Astronomy, California Institute of Technology, Pasadena, CA 91125, USA 6 Institute for Astronomy, University of Hawai‘iatMānoa, Hilo, HI 96720-2700, USA 7 GMTO Corp., 251 S. Lake Ave., Pasadena, CA 91101, USA 8 Observatories of the Carnegie Institution for Science, 813 Santa Barbara St., Pasadena, CA 91101, USA 9 Inter-University Centre for Astronomy & Astrophysics, Ganeshkhind, Pune, 411007, India 10 Seismological Laboratory, California Institute of Technology, 1200 E. California Blvd., Pasadena, CA 91101, USA 11 Department of Physics and Astronomy, University of North Carolina at Chapel Hill, Chapel Hill, NC 27599-3255, USA Received 2014 June 20; accepted 2015 February 25; published 2015 March 30 ABSTRACT HD 8673 hosts a massive exoplanet in a highly eccentric orbit (e = 0.723). Based on two epochs of speckle interferometry a previous publication identified a candidate stellar companion. We observed HD 8673 multiple times with the 10 m Keck II telescope, the 5 m Hale telescope, the 3.63 m Advanced Electro-Optical System telescope, and the 1.5 m Palomar telescope in a variety of filters with the aim of confirming and characterizing the stellar companion. We did not detect the candidate companion, which we now conclude was a false detection, but we did detect a fainter companion. We collected astrometry and photometry of the companion on six epochs in a variety of filters. The measured differential photometry enabled us to determine that the companion is an early M dwarf with a mass estimate of 0.33–0.45 M. The companion has a projected separation of 10 AU, which is one of the smallest projected separations of an exoplanet host binary system. Based on the limited astrometry collected, we are able to constrain the orbit of the stellar companion to a semimajor axis of 35–60 AU, an eccentricity ⩽0.5, and an inclination of 75°–85°. The stellar companion has likely strongly influenced the orbit of the exoplanet and quite possibly explains its high eccentricity. Key words: binaries: visual – instrumentation: adaptive optics – stars: individual (HD 8673) – stars: late-type 1. INTRODUCTION A substellar companion orbiting HD 8673 was detected via radial velocity (RV) measurements by Hartmann et al. (2010). HD 8673 (HR 410 = HIP 6702 = WDS 01262+3435) is HD 8673b has a minimum mass of 14.2 ± 1.6 M , suggested identified as a member of the larger Hyades Moving Group Jup fi that it is probably a low-mass brown dwarf rather than a planet. although it does not t the Hyades Li-temperature pattern or the ( = ± ) ( ) The companion is in a high eccentricity e 0.723 0.016 Hyades Fe abundances Boesgaard & Budge 1988 . There is a ± ( ) orbit with a period of 1634 17 days. The orbit has a spread in the age estimates of the star. Saffe et al. 2005 ± +0.5 semimajor axis of 3.02 0.15 AU. The detection was part of derived an age of 2.8-0.7 Gyr from isochrones and an age of ( ) an effort to detect sub-stellar companions to F-type stars in 8.7 Gyr from Fe/H abundances. Holmberg et al. 2009 order to increase the statistics of exoplanets around stars more produced a similar age of 2.5 Gyr using the photometric massive than the Sun. ( ) technique. Using isochrones, Valenti & Fischer 2005 , In an earlier paper, we described a candidate stellar computed an age of 4.29 Gyr. This variation in age estimates companion to HD 8673 (Mason et al. 2011). In order to ( ) is normal due to a number of factors Saffe et al. 2005 and confirm the candidate companion and determine the impact of HD 8673 is probably somewhere in age between the Hyades the stellar companion on the orbital dynamics of the planetary and the Sun. It can be broadly described as a nearby solar type system, we conducted a series of adaptive optics (AO) fi ( star. It was spectroscopically classi ed as an F7V Boesgaard observations using four different telescopes. Those observa- & Friel 1990) and has a distance of 36.1 ± 0.5 pc (van tions now lead us to conclude that our previous detection was Leeuwen 2007). Tsantaki et al. (2014) computed that it had a spurious. However, we detected another companion that ± ± Teff of 6472 64, a mass of 1.56 0.10 M, and a radius of appears to be a bound low-mass stellar companion in a 1.23 ± 0.07 R. century-long orbit. Details of the observations are in Section 2, and the analysis of the companion is detailed in Section 3. 12 Deceased. Finally we discuss the system in Section 4. 1 The Astronomical Journal, 149:144 (6pp), 2015 April Roberts et al. Table 1 bars were assigned using the technique described in Roberts Astrometry et al. (2005). The resulting astrometry and photometry are UT θ (°) ρ (″) Telescope listed in Tables 1 and 2. Figure 2 shows an image from the 2013 data collection. 2004.7871 302.3 ± 1.0 0.31 ± 0.02 AEOS 2011.5366 332.3 ± 1.0 0.310 ± 0.005 Keck II 2011.6402 329.5 ± 1.0 0.308 ± 0.1 Hale 2011.8671 333.4 ± 0.57 0.308 ± 0.003 Keck II 2.3. AEOS Observations ± ± 2012.4837 335.2 0.63 0.308 0.003 Keck II Following the Keck II and Hale resolutions, archival 2013.7426 339.3 ± 1.68 0.32 ± 0.02 Hale observations obtained with the AEOS 3.67 m telescope (Vigil et al. 1996) were re-examined for a comparable companion 2. OBSERVATIONS detection. On 2004 October 14 UT the star was observed in an effort to detect the bright companion detected by Mason et al. We observed HD 8673 with four telescopes, each equipped (2011). The observations used the telescope’s AO system and with AO. Two of the AO systems operate in the visible, while the Visible Imager camera (Roberts & Neyman 2002).We two operate in the near-IR. collected 1000 frames of the star with the Bessel I filter. After debiasing, dark subtraction, and flat fielding, the resulting 2.1. Keck II Observations frames were coadded with each frame weighted by its peak We used the Keck II telescope, its AO system (Wizinowich pixel to emphasize the best quality data. The result is shown in et al. 2000), and the NIRC2 instrument to observe the system at Figure 3. The companion is harder to see than in the Keck II or three epochs in 2011 and 2012. Each time, we collected data in Hale images, due to a lower image quality because of the multiple filters with multiple coadds. Since the existence of the shorter wavelength and because the system has a larger companion was still questionable, the multiple filters allowed dynamic range in the I filter. us to determine if the object was an astronomical object or a Again, we measured the astrometry and photometry with the quasi-static speckle whose position is wavelength dependent. iterative blind deconvolution algorithm, fitstars. Photometric The 2012 Brγ image of HD 8673 and its companion is shown error bars were assigned using the technique described in in Figure 1. Roberts et al. (2005). Tables 1 and 2 list the resulting After reducing each image, we measured the astrometry and astrometry and photometry measurements. photometry using the fitstars algorithm on each image (ten Brummelaar et al. 1996, 2000). Photometric error bars were set equal to the standard deviation of the measurements from all 2.4. Palomar 1.5 M Observations the images. We computed the weighted mean of the astrometry from the images taken in different filters on the same night, In 2012 and 2013, we observed HD 8673 four times with the with the weight being the number of coadds for each image. Robo-AO system (Baranec et al. 2013, 2014) on the Palomar The error bar was set to the standard deviation of the results. 1.5 m telescope. On 2012 July 17 UT and 2012 July 18 UT, we That covers much of the random errors, but does not cover the used the SDSS r’, i’, z’ filters, on 2012 October 6 UT we used systematic errors. We expect those to be smaller than those of the SDSS i’ and g’ filters, and on 2013 January 20 UT we used the Advanced Electro-Optical System (AEOS; Section 2.3) or the SDSS r’, i’, z’ filters. In 2012, the observations were ( ) Hale data Section 2.2 because of the smaller point-spread collected as part of the automated Robo-AO target queue, ( ) function PSF arising from the larger aperture size, but we do where the telescope is pointed at the object robotically with a not have a way of quantifying those errors.

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