2009/12/31 by E. K. Simpson, D. Pollacco, G. Hébrard +10 · 31 citations
Physics and Astronomy · #Astronomy #Astronomy and Astrophysical Research #Astrophysics #Astrophysics and Star Formation Studies #Exoplanet #Geometry #Line (geometry) #Orbit (dynamics) #Physics #Planet #Planetary system #Radial velocity #Spectral line #Spectrograph #Stars #Stellar rotation #Stellar, planetary, and galactic studies #Transit (satellite) #astro-ph.EP
paper · pdf · open access · doi:10.1111/j.1365-2966.2010.16576.x
published in Monthly Notices of the Royal Astronomical Society (Oxford University Press) · 7 pages, 3 figures, published in MNRAS 405 (2010) 1867-1872. Update includes discussion on differential rotaation and correction of typos
openalex publication_date 2010/04/01 · arxiv created 2010/06/28 · arxiv updated 2014/11/20 · openalex created_date 2020/11/23 · openalex updated_date 2026/08/05
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).