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Figure 1: Comparison of the photometric precision for aperture photometry with neighbor subtraction (Ap) and for PSF fitting photometry (PSF) as a function of the apparent visual magnitude for CFHT, SPM, Loiano and NOT images. The short dashed line indicates the N/S considering only the star photon noise, the long dashed line is the N/S due to the sky photon noise and the detector noise. The continuous line is the total N/S. |
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Figure 2: Comparison of the photometric precision for image subtraction (ISIS) and for psf fitting photometry (PSF) as function of the apparent visual magnitude for CFHT, SPM, Loiano, and NOT images. |
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Figure 3: The expected rms noise for the observations taken at the different sites as a function of the visual apparent magnitude, is compared with the rms of the observed light curves obtained with the image subtraction technique. |
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Figure 4: rms noise for the San Pedro Mártir observations with the aperture error (triangles) as estimated by Eq. (3). |
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Figure 5: The NGC 6791 CMD highlighting the selection region of the main sequence stars (blue circles). |
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Figure 6: False Alarm Probability (FAR) in %, against the DSP parameter given by the algorithm. The points indicate the results of our simulations on constant light curves, the solid line is our assumed best fit. |
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Figure 7: CMD diagram of NGC6791 with the best fit Z=0.030 isochrone (dashed line), and the best fit Z=0.046 isochrone (from Carraro et al. 2006, solid line). Photometry: Stetson et al. (2003) |
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Figure 8:
Left:
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Figure 9: Continuous line: adopted distribution for planet periods. Histogram: RV surveys data (from the Extrasolar Planets Encyclopaedia). |
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Figure 10: Top: constant light curve. Bottom: the same light curve after inserting the simulated transit with limb-darkening (black points). The solid line shows the theoretical light curve of the transit. |
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Figure 11:
TDE as a function of the stellar magnitude for various assumptions
on planetary radii distribution.
From the top to the bottom: 1) Dashed line,
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Figure 12:
( Upper left) Distributions of transit depths measured by the BLS algorithm on the artificial constant-light-curves (lc); ( upper right) transit depths measured on artificial light curves with transits
added; ( lower left) input transit depths used to generate
artificial light curves with transits; ( lower right) relative
difference between the transit depth recovered by BLS
and its input value. Empty histograms refer to distributions relative to all light curves, filled ones to light curves with totally and
partially recovered transits. Histograms are normalized
to all light curves with transiting planets, or,
for the upper left panel to all constant light curves.
This figure is relative to CFHT data, and the assumed
planetary radii distribution is
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Figure 13: The same as Fig. 12 for the transit periods. |
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Figure 14: The same as Fig.12 for the transit durations. |
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Figure 15:
Composite light curve of candidate 6598. In ordinate
is reported the calibrated V magnitude and in abscissa the observing epoch,
(in days), where 0 corresponds to
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Figure 16: Composite light curve of candidate 4304. |
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Figure 17: Composite light curve of candidate 4699. |
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Figure 18: CFHT light curve for candidate 1239. |
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Figure 19: CFHT light curve for candidate 4300. |
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Figure 20: CFHT light curve for candidate 7591. |
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Figure 21: Composite light curve for candidate 3671 correspondent to T5 of BO3. Different symbols have the same meaning of Fig. 15. |
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Figure 22: Composite light curve for candidate 3723 correspondent to T7 of BO3. |
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Figure 23: Composite light curve for candidate 12390 correspondent to T9 of BO3. |
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