J/AJ/152/127       Sloan i follow-up light curves of HATS-18      (Penev+, 2016)
HATS-18b: an extreme short-period massive transiting planet spinning up its
star.
    Penev K., Hartman J.D., Bakos G.A., Ciceri S., Brahm R., Bayliss D.,
    Bento J., Jordan A., Csubry Z., Bhatti W., de Val-Borro M., Espinoza N.,
    Zhou G., Mancini L., Rabus M., Suc V., Henning T., Schmidt B., Noyes R.W.,
    Lazar J., Papp I., Sari P.
   <Astron. J., 152, 127-127 (2016)>
   =2016AJ....152..127P 2016AJ....152..127P    (SIMBAD/NED BibCode)
ADC_Keywords: Planets ; Stars, double and multiple ; Photometry, ugriz ;
              Radial velocities
Keywords: planetary systems - planets and satellites: detection -
          planets and satellites: gaseous planets - stars: individual: HATS-18 -
          stars: rotation - techniques: photometric
Abstract:
    We report the discovery by the HATSouth network of HATS-18b: a
    1.980±0.077MJ, 1.337-0.049+0.102RJ planet in a 0.8378day
    orbit, around a solar analog star (mass 1.037±0.047M☉ and
    radius 1.020-0.031+0.057R☉) with V=14.067±0.040mag. The
    high planet mass, combined with its short orbital period, implies
    strong tidal coupling between the planetary orbit and the star. In
    fact, given its inferred age, HATS-18 shows evidence of significant
    tidal spin up, which together with WASP-19 (a very similar system)
    allows us to constrain the tidal quality factor for Sun-like stars to
    be in the range of 6.5≲log10(Q*/k2)≲7 even after allowing for
    extremely pessimistic model uncertainties. In addition, the HATS-18
    system is among the best systems (and often the best system) for
    testing a multitude of star-planet interactions, be they
    gravitational, magnetic, or radiative, as well as planet formation and
    migration theories.
Description:
    The star HATS-18 was observed by HATSouth instruments between UT 2011
    April 18 and UT 2013 July 21 using the HS-2, HS-4, and HS-6 units at
    the Las Campanas Observatory in Chile, the High Energy Spectroscopic
    Survey (H.E.S.S.) site in Namibia, and Siding Spring Observatory (SSO)
    in Australia, respectively. A total of 5372, 3758, and 4008 images of
    HATS-18 were obtained with HS-2, HS-4, and HS-6, respectively. The
    observations were obtained through a Sloan r filter with an exposure
    time of 240s.
    We obtained follow-up light curves of HATS-18 using the Las Cumbres
    Observatory Global Telescope (LCOGT) 1m telescope network. An ingress
    was observed on UT 2015 July 18 with the SBIG camera and a Sloan i
    filter on the 1m at the South African Astronomical Observatory (SAAO).
    A total of 33 images were collected at a median cadence of 201s. A
    full transit was observed on UT 2016 January 22 with the sinistro
    camera and a Sloan i filter on the 1m at Cerro Tololo Inter-American
    Observatory. A total of 61 images were collected at a median cadence
    of 219s. For the record, we also note that a full transit was observed
    on UT 2016 January 3 with the SBIG camera on the 1m at SAAO; however,
    due to tracking and weather problems, we were unable to extract
    high-precision photometry from these images, and therefore do not
    include these data in our analysis. The data are available in Table1.
    Spectroscopic follow-up observations of HATS-18 were carried out with
    WiFeS on the Australian National University (ANU) 2.3m telescope and
    with the Fiber-fed Extended Range Optical Spectrograph (FEROS) on the
    MPG 2.2m. A total of three spectra were obtained with WiFeS between UT
    2015 February 28 and UT 2015 March 2, two at a resolution of
    R=Δλ/λ=7000, and one at R=3000. We obtained six
    R=48000 spectra with FEROS between UT 2015 June 12 and UT 2015 June
    20. The data are provided in Table2.
Objects:
    ---------------------------------------------------------------------
         RA   (ICRS)   DE        Designation(s)            (Period)
    ---------------------------------------------------------------------
     11 35 49.78   -29 09 21.6   HATS-18 = GSC 06664-00410 (P=0.83784340)
    ---------------------------------------------------------------------
File Summary:
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 FileName    Lrecl    Records    Explanations
--------------------------------------------------------------------------------
ReadMe          80          .    This file
table1.dat      58      13232    Differential photometry of HATS-18
table2.dat      55          6    Relative radial velocities and bisector span
                                  measurements of HATS-18
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See also:
 J/AJ/148/29    : Spectroscopy and photometry of HATS-4 (Jordan+, 2014)
 J/AJ/146/113   : Differential griz photometry of HATS-3 (Bayliss+, 2013)
 J/AJ/145/5     : Follow-up photometry of HATS-1 (Penev+, 2013)
 J/AJ/144/139   : HAT-P-39, HAT-P-40, and HAT-P-41 follow-up (Hartman+, 2012)
 J/ApJ/710/1724 : Follow-up photometry for HAT-P-11 (Bakos+, 2010)
Byte-by-byte Description of file: table1.dat
--------------------------------------------------------------------------------
   Bytes Format Units   Label  Explanations
--------------------------------------------------------------------------------
   1- 13  F13.5 d       BJD    UTC Barycentric Julian date (BJD-2400000) (1)
  15- 22  F8.5  mag     Dmag   [-0.073/0.0667] Δ magnitude observed in
                                filter (2)
  24- 30  F7.5  mag   e_Dmag   [0.0016/0.022] Uncertainty in Dmag
  32- 39  F8.5  mag     omag   [-0.009/13.8]? Raw, observed magnitude (3)
      41  A1    ---     Flt    [ir] Filter used in the observation (Sloan i, or
                                Sloan r)
  43- 58  A16   ---     Inst   Instrument used in the observation (HS,
                                LCOGT1m/SBIG, or LCOGT1m/sinistro) (4)
--------------------------------------------------------------------------------
Note (1): Barycentric Julian Date is computed directly from the UTC time without
     correction for leap seconds.
Note (2): The out-of-transit level has been subtracted. For the HATSouth light
     curve (rows with "HS" in the Instrument column), these magnitudes have been
     detrended using the External Parameter Decorrelation (EPD; Bakos et al.
     2010, Cat. J/ApJ/710/1724) and the Trend Filtering Algorithm (TFA; Kovacs
     et al. 2005MNRAS.356..557K 2005MNRAS.356..557K) procedures prior to fitting a transit model
     to the light curve. We apply the TFA in signal-reconstruction mode so as to
     preserve the transit depth. For the follow-up light curves (rows with an
     Instrument other than "HS") these magnitudes have been detrended with the
     EPD procedure, carried out simultaneously with the transit fit.
Note (3): Raw magnitude values without application of the EPD procedure. This is
     only reported for the follow-up light curves.
Note (4): The instruments used are defined as follows:
     HS               = HATSouth telescope;
     LCOGT1m/SBIG     = Las Cumbres Observatory Global Telescope (LCOGT) 1m
                        telescope + Siding Spring Observatory (SSO)/SBIG camera;
     LCOGT1m/sinistro = LCOGT 1m telescope + Cerro Tololo Inter-American
                        Observatory (CTIO)/sinistro camera.
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Byte-by-byte Description of file: table2.dat
--------------------------------------------------------------------------------
   Bytes Format Units   Label     Explanations
--------------------------------------------------------------------------------
   1- 13  F13.5 d       BJD       Barycentric Julian Date (1)
  15- 21  F7.2  m/s     RV        [-420.1/425] Relative radial velocity (2)
  23- 27  F5.2  m/s   e_RV        [15/21] Uncertainty in RV (3)
  29- 34  F6.2  m/s     BS        [-24/149] Bisector span
  36- 40  F5.2  m/s   e_BS        [16/24] Uncertainty in BS
  42- 49  F8.6  ---     Phase     [0/1] Phase
  51- 55  A5    ---     Inst      Instrument (FEROS=Fiber-fed Extended Range
                                   Optical Spectrograph/MPG 2.2m)
--------------------------------------------------------------------------------
Note (1): Barycentric Julian Date is computed directly from the UTC time without
     correction for leap seconds.
Note (2): Relative radial velocity, with γRV subtracted (See Table3).
Note (3): Internal errors excluding the component of astrophysical/instrumental
     jitter considered in Section 3 in the paper.
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History:
    From electronic version of the journal
(End)                 Prepared by [AAS]; Sylvain Guehenneux [CDS]    02-Feb-2017