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Table 1

Summary of photometric observations.

Instrument/fielda UT date(s) # Images Cadenceb Filter Precisionc
(s) (mmag)

HATS-13
HS-2/G582 2009 Nov.–2010 Sep. 2486 288 r 12.6
HS-4/G582 2009 Sep.–2010 Sep. 8565 288 r 12.2
HS-6/G582 2010 Apr.–2010 Sep. 356 265 r 13.1
CTIO 0.9 md 2012 Aug. 26 68 237 z 2.9
MPG 2.2 m/GRONDd 2012 Oct. 17 82 87 g 1.4
MPG 2.2 m/GRONDd 2012 Oct. 17 83 87 r 1.2
MPG 2.2 m/GRONDd 2012 Oct. 17 82 87 i 1.7
MPG 2.2 m/GRONDd 2012 Oct. 17 82 87 z 1.6
PEST 2013 May 3 99 130 R 4.7
PEST 2013 Jun. 30 189 130 R 4.7
HATS-14
HS-2/G582 2009 Nov.–2010 Sep. 4866 284 r 11.5
HS-4/G582 2009 Sep.–2010 Sep. 8889 288 r 12.6
HS-6/G582 2010 Aug.–2010 Sep. 200 290 r 11.6
PEST 2013 Jun. 06 131 131 R 4.8
MPG 2.2 m/GRONDd 2013 Jun. 12 114 192 g 1.6
MPG 2.2 m/GRONDd 2013 Jun. 12 114 192 r 1.8
MPG 2.2 m/GRONDd 2013 Jun. 12 114 192 i 2.6
MPG 2.2 m/GRONDd 2013 Jun. 12 114 192 z 2.0

Notes.

(a)

For HATSouth data we list the HATSouth unit and field name from which the observations are taken. HS-1 and -2 are located at Las Campanas Observatory in Chile, HS-3 and -4 are located at the HESS site in Namibia, and HS-5 and -6 are located at Siding Spring Observatory in Australia. Each field corresponds to one of 838 fixed pointings used to cover the full 4π celestial sphere. All data from a given HATSouth field are reduced together, while detrending through External Parameter Decorrelation (EPD) is done independently for each unique field+unit combination.

(b)

The median time between consecutive images rounded to the nearest second. Due to weather, the day-night cycle, guiding and focus corrections, and other factors, the cadence is only approximately uniform over short timescales.

(c)

The root mean square of the residuals from the best-fit model.

(d)

The telescope-defocussing technique (Southworth et al. 2009) was used for this transit observation.

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