HATS-13b and HATS-14b: two transiting hot Jupiters from the HATSouth survey

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Volume 580 (August 2015)

A&A, 580 (2015) A63

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Table A.1

Light curve data for HATS-13and HATS-14.

Object^a	BJD^b	Mag^c	σ _Mag	Mag(orig)^d	Filter	Instrument
	(2 400 000+)

HATS-13	55 419.49174	−0.01156	0.00605	0.00000	r	HS
HATS-13	55 434.71221	−0.00680	0.00753	0.00000	r	HS
HATS-13	55 413.40415	0.00030	0.00605	0.00000	r	HS
HATS-13	55 416.44831	0.00714	0.00620	0.00000	r	HS
HATS-13	55 352.52327	0.01857	0.00631	0.00000	r	HS
HATS-13	55 422.53650	−0.00515	0.00599	0.00000	r	HS
HATS-13	55 355.56742	0.00957	0.00621	0.00000	r	HS
HATS-13	55 291.64236	0.02224	0.00758	0.00000	r	HS
HATS-13	55 373.83182	0.01939	0.00907	0.00000	r	HS
HATS-13	55 361.65578	−0.00370	0.00583	0.00000	r	HS

Notes.This table is available in a machine-readable form at the CDS. A portion is shown here for guidance regarding its form and content.

^(a)

Either HATS-13, or HATS-14.

^(b)

Barycentric Julian Date is computed directly from the UTC time without correction for leap seconds.

^(c)

The out-of-transit level has been subtracted. For observations made with the HATSouth instruments (identifed by “HS” in the “Instrument” column), these magnitudes have been corrected for trends using the EPD and TFA procedures applied prior to fitting the transit model. This procedure may lead to an artificial dilution in the transit depths. For HATS-13, the transit depth is 95% of the true depth, with for HATS-14it is 93% of the true depth. For observations made with follow-up instruments (anything other than “HS” in the “Instrument” column), the magnitudes have been corrected for a quadratic trend in time fit simultaneously with the transit.

^(d)

Raw magnitude values without correction for the quadratic trend in time. These are only reported for the follow-up observations.

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