Detection of period variations in extrasolar transiting planet OGLE-TR-111b
Summary (1 min read)
2. OBSERVATIONS AND DATA REDUCTION
- The authors observed two consecutive transits of planetary companion OGLE-TR-111b in the I band with the FORS1 instrument at the European Southern Observatory (ESO) Very Large Telescope (VLT).
- For the observations, a nearby bright star was moved outside the field of view, leaving OGLE-TR-111 near the center of the north-eastern quadrant.
- Aperture photometry was performed on the difference images using IRAF DAOPHOT package (Stetson 1987), which was found to give better results than the ISIS photometry routine phot.csh (for a detailed description of the ISIS routines see Hartman et al. 2004).
- In the same paper Kovács et al. (2005) present an iterative method to reconstruct signals affected by systematics effects, based on the TFA method.
- The standard deviation before the transit of the second night is 2.65 mmag, almost reaching the photon noise limit of 2.55 mmag.
3. MEASUREMENTS
- Planetary and orbital parameters, including the central times of transits, were fitted to the OGLE-TR-111 light curve.
- The uncertainties in the parameters were estimated using the Markov Chain Monte Carlo method, which is described in detail by Tegmark et al. (2004), Ford (2005) and Holman et al. (2006).
- Possible systematic errors may be introduced by the choice of the stellar mass, the orbital period — which affects the determination of the orbital radius—, the model for the limb darkening, and the flux in the reference image.
- The coefficients for the quadratic limb-darkenning model were adjusted from the data instead of fixed to the values of Claret (2000) and, additionally, a linear limb darkenning model was considered, both fixing the linear coefficient to the value computed by Claret (2000) and adjusting it as part of the fit.
- The authors therefore conclude that the values obtained for the central transit times are robust.
4. RESULTS AND DISCUSSION
- In Fig. 3 the authors present the observed-minus-computed (O-C) times for the two transits together with those from W07 and Minniti et al. (2007).
- The central time of this last transit has been remeasured using the procedure described above, which is different from the one employed in the original paper, to reduce any effects produced by differing techniques.
- The authors have been able to discard a few possibilities and study some others.
- On the other hand, the mass of the perturber planet must be around 5 MJup if the orbit of the interior planet is nearly circular.
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Frequently Asked Questions (12)
Q2. What have the authors stated for future works in "Detection of period variations in extrasolar transiting planet" ?
The authors present some preliminary results here and defer a more detailed study for a future work.
Q3. How many stars were used as template light curves?
The authors obtained photometry of 19 stars distributed as uniformly as possible around OGLE-TR-111to use as template light curves for the TFA.
Q4. How was the signal reconstruction algorithm used?
The signal-reconstruction algorithm was iterated until the relative difference in the curves obtained in two successive steps was less than 10−5.
Q5. How many mmags is the standard deviation before the transit of the second night?
1. The standarddeviation before the transit of the second night is 2.65 mmag, almost reaching the photon noise limit of 2.55 mmag.
Q6. How many days were the O-C times calculated?
(1)The O-C times were computed using the ephemeris for the planetary transits presentedby W07:Tc = 2453799.7516± 0.0002 [HJD] (2) P = 4.0144479± 0.0000041 days .
Q7. What was the fit for the quadratic limb-darkenning model?
The coefficients for the quadratic limb-darkenning model were adjusted from the data instead of fixed to the values of Claret (2000) and, additionally, a linear limb darkenning model was considered, both fixing the linear coefficient to the value computed by Claret (2000) and adjusting it as part of the fit.
Q8. How far from the moon is the moon from the planet?
the hypothesis of an exomoon seems unlikely, since the mass needed to producethe observed O-C times is at least a twentieth of the planetary mass if the moon is at a Hill radius from the planet.
Q9. Why did the authors choose a 5-pixels aperture?
The authors therefore choose a 5-pixels aperture since their goal is to obtain precise measurements of the central times of transits, and therefore the relevance of obtaining the correct amplitude is diminished.
Q10. What are the possible errors in the limbs?
Possible systematic errors may be introduced by the choice of the stellar mass, theorbital period — which affects the determination of the orbital radius—, the model for the limb darkening, and the flux in the reference image.
Q11. What is the fit for the limb-darkening?
The authors considered a quadratic model for the limb-darkening, with coefficients taken from Claret (2000) for a star with Teff = 5000 K, log g = 4.5 cm s −2 and [Fe/H] = 0.2 and microturbulent velocity ξ = 2 km/s.
Q12. How did Deeg and Ribas find the planets?
Deeg et al. (2008) and Ribas et al. (2008) reported indirect detections of unseen companions by monitoring eclipse timing of the binary stellar system CM Draconis (1.5 MJ to 0.1 M candidate) and variations in the orbital parameters of the planetary system around GJ 436 (5 M⊕ companion), respectively.