A. Vidal-Madjar
Institut d'Astrophysique de Paris
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Featured researches published by A. Vidal-Madjar.
Nature | 2003
A. Vidal-Madjar; A. Lecavelier des Etangs; J.-M. Désert; G. Ballester; R. Ferlet; G. Hébrard; M. Mayor
The planet in the system HD209458 is the first one for which repeated transits across the stellar disk have been observed. Together with radial velocity measurements, this has led to a determination of the planets radius and mass, confirming it to be a gas giant. But despite numerous searches for an atmospheric signature, only the dense lower atmosphere of HD209458b has been observed, through the detection of neutral sodium absorption. Here we report the detection of atomic hydrogen absorption in the stellar Lyman α line during three transits of HD209458b. An absorption of 15 ± 4% (1σ) is observed. Comparison with models shows that this absorption should take place beyond the Roche limit and therefore can be understood in terms of escaping hydrogen atoms.
The Astrophysical Journal | 2000
H. W. Moos; Webster Cash; L. L. Cowie; Arthur F. Davidsen; Andrea K. Dupree; Paul D. Feldman; Scott D. Friedman; James C. Green; R. F. Green; C. Gry; J. B. Hutchings; Edward B. Jenkins; J. L. Linsky; Roger F. Malina; Andrew G. Michalitsianos; Blair D. Savage; J. M. Shull; O. H. W. Siegmund; Theodore P. Snow; George Sonneborn; A. Vidal-Madjar; Allan J. Willis; Bruce E. Woodgate; D. G. York; Thomas B. Ake; B-G Andersson; John Paul Andrews; Robert H. Barkhouser; Luciana Bianchi; William P. Blair
The Far Ultraviolet Spectroscopic Explorer satellite observes light in the far-ultraviolet spectral region, 905-1187 Angstrom, with a high spectral resolution. The instrument consists of four co-aligned prime-focus telescopes and Rowland spectrographs with microchannel plate detectors. Two of the telescope channels use Al :LiF coatings for optimum reflectivity between approximately 1000 and 1187 Angstrom, and the other two channels use SiC coatings for optimized throughput between 905 and 1105 Angstrom. The gratings are holographically ruled to correct largely for astigmatism and to minimize scattered light. The microchannel plate detectors have KBr photocathodes and use photon counting to achieve good quantum efficiency with low background signal. The sensitivity is sufficient to examine reddened lines of sight within the Milky Way and also sufficient to use as active galactic nuclei and QSOs for absorption-line studies of both Milky Way and extragalactic gas clouds. This spectral region contains a number of key scientific diagnostics, including O VI, H I, D I, and the strong electronic transitions of H-2 and HD.
Nature | 1993
E. Aubourg; P. Bareyre; S. Brehin; Michel Gros; Marc Lachieze-Rey; Beatrice St. Laurent; E. Lesquoy; C. Magneville; A. Milsztajn; Luciano Moscoso; F. Queinnec; J. Rich; Michel Spiro; L. Vigroux; S. Zylberajch; R. Ansari; F. Cavalier; M. Moniez; J. P. Beaulieu; R. Ferlet; Ph. Grison; A. Vidal-Madjar; J. Guibert; Olivier Moreau; F. Tajahmady; E. Maurice; L. Prevot; C. Gry
THE flat rotation curves of spiral galaxies, including our own, indicate that they are surrounded by unseen haloes of ‘dark matter’1,2. In the absence of a massive halo, stars and gas in the outer portions of a galaxy would orbit the centre more slowly, just as the outer planets in the Solar System circle the Sun more slowly than the inner ones. So far, however, there has been no direct observational evidence for the dark matter, or its characteristics. Paczyński3suggested that dark bodies in the halo of our Galaxy can be detected when they act as gravitational ‘microlenses’, amplifying the light from stars in nearby galaxies. The duration of such an event depends on the mass, distance and velocity of the dark object. We have been monitoring the brightness of three million stars in the Large Magellanic Cloud for over three years, and here report the detection of two possible microlensing events. The brightening of the stars was symmetrical in time, achromatic and not repeated during the monitoring period. The timescales of the two events are about thirty days and imply that the masses of the lensing objects lie between a few hundredths and one solar mass. The number of events observed is consistent with the number expected if the halo is dominated by objects with masses in this range.
Nature | 2007
Giovanna Tinetti; A. Vidal-Madjar; Mao-Chang Liang; Jean-Philippe Beaulieu; Yuk L. Yung; Sean J. Carey; Robert J. Barber; Jonathan Tennyson; Ignasi Ribas; Nicole F. Allard; G. E. Ballester; David Kent Sing; Franck Selsis
Water is predicted to be among the most abundant (if not the most abundant) molecular species after hydrogen in the atmospheres of close-in extrasolar giant planets (‘hot Jupiters’). Several attempts have been made to detect water on such planets, but have either failed to find compelling evidence for it or led to claims that should be taken with caution. Here we report an analysis of recent observations of the hot Jupiter HD 189733b (ref. 6) taken during the transit, when the planet passed in front of its parent star. We find that absorption by water vapour is the most likely cause of the wavelength-dependent variations in the effective radius of the planet at the infrared wavelengths 3.6 μm, 5.8 μm (both ref. 7) and 8 μm (ref. 8). The larger effective radius observed at visible wavelengths may arise from either stellar variability or the presence of clouds/hazes. We explain the report of a non-detection of water on HD 189733b (ref. 4) as being a consequence of the nearly isothermal vertical profile of the planet’s atmosphere.
The Astrophysical Journal | 2002
Brian L. Rachford; Theodore P. Snow; Jason Tumlinson; J. M. Shull; William P. Blair; Roger Ferlet; Scott D. Friedman; C. Gry; Edward B. Jenkins; Donald C. Morton; Blair D. Savage; Paule Sonnentrucker; A. Vidal-Madjar; Daniel E. Welty; D. G. York
We report the first ensemble results from the Far Ultraviolet Spectroscopic Explorer survey of molecular hydrogen in lines of sight with AV e1 mag. We have developed techniques for fitting computed profiles to the low-J lines of H2, and thus determining column densities for J ¼ 0 and J ¼ 1, which contain e99% of the total H2. From these column densities and ancillary data we have derived the total H2 column densities, hydrogen molecular fractions, and kinetic temperatures for 23 lines of sight. This is the first significant sample of molecular hydrogen column densities of � 10 21 cm � 2 , measured through UV absorption bands. We have also compiled a set of extinction data for these lines of sight, which sample a wide range of environments. We have searched for correlations of our H2-related quantities with previously published column densities of other molecules and extinction parameters. We find strong correlations between H2 and molecules such as CH, CN, and CO, in general agreement with predictions of chemical models. We also find the expected correlations between hydrogen molecular fraction and various density indicators such as kinetic temperature, CN
Nature | 2016
David K. Sing; Jonathan J. Fortney; N. Nikolov; Hannah R. Wakeford; Tiffany Kataria; T. Evans; Suzanne Aigrain; G. E. Ballester; Adam Burrows; Drake Deming; Jean-Michel Desert; N. P. Gibson; Gregory W. Henry; Catherine M. Huitson; Heather A. Knutson; Alain Lecavelier des Etangs; F. Pont; A. Vidal-Madjar; Michael H. Williamson; Paul A. Wilson
Thousands of transiting exoplanets have been discovered, but spectral analysis of their atmospheres has so far been dominated by a small number of exoplanets and data spanning relatively narrow wavelength ranges (such as 1.1–1.7 micrometres). Recent studies show that some hot-Jupiter exoplanets have much weaker water absorption features in their near-infrared spectra than predicted. The low amplitude of water signatures could be explained by very low water abundances, which may be a sign that water was depleted in the protoplanetary disk at the planet’s formation location, but it is unclear whether this level of depletion can actually occur. Alternatively, these weak signals could be the result of obscuration by clouds or hazes, as found in some optical spectra. Here we report results from a comparative study of ten hot Jupiters covering the wavelength range 0.3–5 micrometres, which allows us to resolve both the optical scattering and infrared molecular absorption spectroscopically. Our results reveal a diverse group of hot Jupiters that exhibit a continuum from clear to cloudy atmospheres. We find that the difference between the planetary radius measured at optical and infrared wavelengths is an effective metric for distinguishing different atmosphere types. The difference correlates with the spectral strength of water, so that strong water absorption lines are seen in clear-atmosphere planets and the weakest features are associated with clouds and hazes. This result strongly suggests that primordial water depletion during formation is unlikely and that clouds and hazes are the cause of weaker spectral signatures.
Astronomy and Astrophysics | 2008
A. Lecavelier des Etangs; F. Pont; A. Vidal-Madjar; David K. Sing
The transit spectrum of the exoplanet HD 189733b has recently been obtained between 0.55 and 1.05 µm. Here we present an analysis of this spectrum. We develop first-order equations to interpret absorption spectra. In the case of HD 189733b, we show that the observed slope of the absorption as a function of wavelength is characteristic of extinction proportional to the inverse of the fourth power of the wavelength (∝λ −4 ). Assuming an extinction dominated by Rayleigh scattering, we derive an atmospheric temperature of 1340 ± 150 K. If molecular hydrogen is responsible for the Rayleigh scattering, the atmospheric pressure at the planetary characteristic radius of 0.1564 stellar radius must be 410 ± 30 mbar. However the preferred scenario is scattering by condensate particles. Using the Mie approximation, we find that the particles must have a low value for the imaginary part of the refraction index. We identify MgSiO3 as a possible abundant condensate whose particle size must be between ∼10 −2 and ∼10 −1 µm. For this condensate, assuming solar abundance, the pressure at 0.1564 stellar radius is found to be between a few microbars and few millibars, and the temperature is found to be in the range 1340–1540 K, and both depend on the particle size.
The Astrophysical Journal | 2009
J.-M. Désert; Alain Lecavelier des Etangs; G. Hébrard; David K. Sing; D. Ehrenreich; R. Ferlet; A. Vidal-Madjar
Water, methane, and carbon monoxide are expected to be among the most abundant molecules besides molecular hydrogen in the hot atmosphere of close-in extrasolar giant planets. Atmospheric models for these planets predict that the strongest spectrophotometric features of those molecules are located at wavelengths ranging from 1 to 10 ?m? making this region of particular interest. Consequently, transit observations in the mid-infrared (mid-IR) allow the atmospheric content of transiting planets to be determined. We present new primary transit observations of the hot-Jupiter HD?189733b, obtained simultaneously at 4.5 and 8 ?m with the Infrared Array Camera onboard the Spitzer Space Telescope. Together with a new refined analysis of previous observations at 3.6 and 5.8 ?m using the same instrument, we are able to derive the system parameters, including planet-to-star radius ratio, impact parameter, scale of the system, and central time of the transit from fits of the transit light curves at these four wavelengths. We measure the four planet-to-star radius ratios, to be (Rp /R )3.6 ?m = 0.1545 ? 0.0003, (Rp /R )4.5 ?m = 0.1557 ? 0.0003, (Rp /R )5.8 ?m = 0.1547 ? 0.0005, and (Rp /R )8 ?m = 0.1544 ? 0.0004. The high accuracy of the planet radii measurement allows the search for atmospheric molecular absorbers. Contrary to a previous analysis of the same data set, our study is robust against systematics and reveals that water vapor absorption at 5.8 ?m is not detected in this photometric data set. Furthermore, in the band centered around 4.5??m we find a hint of excess absorption with an apparent planetary radius ?Rp /R * = 0.00128 ? 0.00056 larger (2.3?) than the one measured simultaneously at 8??m. This value is 4? above what would be expected for an atmosphere where water vapor is the only absorbing species in the near-IR. This shows that an additional species absorbing around 4.5 ?m could be present in the atmosphere. Carbon monoxide (CO) being a strong absorber at this wavelength is a possible candidate and this may suggest a large CO/H2O ratio between 5 and 60.
Astronomy and Astrophysics | 2008
G. Hébrard; F. Bouchy; F. Pont; B. Loeillet; M. Rabus; Xavier Bonfils; Claire Moutou; I. Boisse; X. Delfosse; M. Desort; Anne Eggenberger; D. Ehrenreich; T. Forveille; Anne-Marie Lagrange; C. Lovis; Michel Mayor; F. Pepe; C. Perrier; D. Queloz; N. C. Santos; D. Ségransan; S. Udry; A. Vidal-Madjar
The transiting extrasolar planet XO-3b is remarkable, with a high mass and eccentric orbit. These unusual characteristics make it interesting to test whether its orbital plane is parallel to the equator of its host star, as it is observed for other transiting planets. We performed radial velocity measurements of XO-3 with the SOPHIE spectrograph at the 1.93 m telescope of Haute-Provence Observatory during a planetary transit and at other orbital phases. This allowed us to observe the Rossiter-McLaughlin effect and, together with a new analysis of the transit light curve, to refine the parameters of the planet. The unusual shape of the radial velocity anomaly during the transit provides a hint of a nearly transverse Rossiter-McLaughlin effect. The sky-projected angle between the planetary orbital axis and the stellar rotation axis should be λ = 70 ◦ ± 15 ◦ to be compatible with our observations. This suggests that some close-in planets might result from gravitational interaction between planets and/or stars rather than migration due to interaction with the accretion disk. This surprising result requires confirmation by additional observations, especially at lower airmass, to fully exclude the possibility that the signal is due to systematic effects.
The Astrophysical Journal | 1998
C. Alcock; Robyn A. Allsman; D. Alves; R. Ansari; E. Aubourg; Tim Axelrod; P. Bareyre; J. P. Beaulieu; Andrew Cameron Becker; D. P. Bennett; S Brehin; F. Cavalier; S. Char; Kem Holland Cook; R. Ferlet; J Fernandez; Kenneth C. Freeman; Kim Griest; Ph. Grison; M. Gros; C. Gry; J Guibert; M Lachieze-Rey; B Laurent; M J Lehner; E. Lesquoy; C. Magneville; S. L. Marshall; E Maurice; A. Milsztajn
The EROS and MACHO collaborations have each published upper limits on the amount of planetary-mass dark matter in the Galactic halo obtained from gravitational microlensing searches. In this Letter, the two limits are combined to give a much stronger constraint on the abundance of low-mass MACHOs. Specifically, objects with masses 10−7 Mm10−3 M make up less than 25% of the halo dark matter for most models considered, and less than 10% of a standard spherical halo is made of MACHOs in the 3.5×10−7 MThe EROS and MACHO collaborations have each published upper limits on the amount of planetary mass dark matter in the Galactic Halo obtained from gravitational microlensing searches. In this paper the two limits are combined to give a much stronger constraint on the abundance of low mass MACHOs.