Issue |
A&A
Volume 545, September 2012
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|
---|---|---|
Article Number | A76 | |
Number of page(s) | 16 | |
Section | Planets and planetary systems | |
DOI | https://doi.org/10.1051/0004-6361/201219608 | |
Published online | 10 September 2012 |
Online material
SOPHIE measurements of KOI-12.
SOPHIE measurements of KOI-131.
SOPHIE measurements of KOI-190.
SOPHIE measurements of KOI-192.
SOPHIE measurements of KOI-197.
SOPHIE measurements of KOI-201.
SOPHIE measurements of KOI-340.
SOPHIE measurements of KOI-418.
SOPHIE measurements of KOI-419.
SOPHIE measurements of KOI-425.
SOPHIE measurements of KOI-607.
SOPHIE measurements of KOI-609.
SOPHIE measurements of KOI-611.
SOPHIE measurements of KOI-698.
SOPHIE measurements of KOI-1786.
Parameters for KOI-419.
Parameters for KOI-698.
Occurrence of hot Jupiter per thousand of stars.
Fig. 7
KOI-419 light-curve (top panel), radial velocities (middle panel) and spectral energy distribution (bottom panel) with the best-combined fit (red or black line). The phase zero corresponds to the periastron epoch. The open circles in the bottom panel correspond to the best model integrated toward the same band-passes as the photometric measurements (red dots). |
|
Open with DEXTER |
Fig. 8
KOI-698 light-curve (top panel), radial velocities (middle panel) and spectral energy distribution (bottom panel) with the best-combined fit (red or black line). The phase zero corresponds to the periastron epoch. The open circles in the bottom panel correspond to the best model integrated toward the same band-passes as the photometric measurements (red dots). The Rossiter-McLaughlin-like effect seen around phase 0.3 and 0.9 is due to the expected variation when the primary and secondary spectra are blended. |
|
Open with DEXTER |
© ESO, 2012
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