Based on observations collected with the SOPHIE spectrograph on the 1.93-m telescope at Observatoire de Haute-Provence (CNRS), France, by the SOPHIE Consortium (program 08B.PNP.SIMP).
The spin–orbit alignment of the transiting exoplanet WASP-3b from Rossiter–McLaughlin observations†
Article first published online: 9 APR 2010
DOI: 10.1111/j.1365-2966.2010.16576.x
© 2010 The Authors. Journal compilation © 2010 RAS
Issue

Monthly Notices of the Royal Astronomical Society
Volume 405, Issue 3, pages 1867–1872, July 2010
Additional Information
How to Cite
Simpson, E. K., Pollacco, D., Hébrard, G., Gibson, N. P., Barros, S. C. C., Boisse, I., Bouchy, F., Cameron, A. C., Miller, G. R. M., Watson, C. A. and Keenan, F. P. (2010), The spin–orbit alignment of the transiting exoplanet WASP-3b from Rossiter–McLaughlin observations. Monthly Notices of the Royal Astronomical Society, 405: 1867–1872. doi: 10.1111/j.1365-2966.2010.16576.x
- †
Publication History
- Issue published online: 23 JUN 2010
- Article first published online: 9 APR 2010
- Accepted 2010 February 20. Received 2010 February 19; in original form 2009 December 18
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Keywords:
- stars: planetary systems;
- stars: individual: WASP-3;
- techniques: radial velocities;
- techniques: photometric
ABSTRACT
We present an observation of the Rossiter–McLaughlin effect for the planetary system WASP-3. Radial velocity measurements were made during transit using the SOPHIE spectrograph at the 1.93-m telescope at Haute-Provence Observatory. The shape of the effect shows that the sky-projected angle between the stellar rotation axis and planetary orbital axis (λ) is small and consistent with zero within
. WASP-3b joins the ∼two-thirds of planets with measured spin–orbit angles that are well aligned and are thought to have undergone a dynamically gentle migration process such as planet–disc interactions. We find a systematic effect which leads to an anomalously high determination of the projected stellar rotational velocity (v sin i= 19.6+2.2−2.1 km s−1) compared to the value found from spectroscopic line broadening (v sin i= 13.4 ± 1.5 km s−1). This is thought to be caused by a discrepancy in the assumptions made in the extraction and modelling of the data. Using a model developed by Hirano et al. designed to address this issue, we find v sin i to be consistent with the value obtained from spectroscopic broadening measurements (v sin i= 15.7+1.4−1.3 km s−1).

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