P. Rousselot
University of Franche-Comté
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Featured researches published by P. Rousselot.
The Astronomical Journal | 2009
Jean-Marc Petit; J. J. Kavelaars; Brett James Gladman; R.L. Jones; J. Wm. Parker; C. Van Laerhoven; P. D. Nicholson; G. Mars; P. Rousselot; Olivier Mousis; B. G. Marsden; Allyson Bieryla; M. Taylor; M. L. N. Ashby; Paula Gabriela Benavídez; A. Campo Bagatin; Guillermo Bernabeu
We report the orbital distribution of the trans-Neptunian objects (TNOs) discovered during the Canada–France Ecliptic Plane Survey (CFEPS), whose discovery phase ran from early 2003 until early 2007. The follow-up observations started just after the first discoveries and extended until late 2009. We obtained characterized observations of 321 deg 2 of sky to depths in the range g ∼ 23.5–24.4 AB mag. We provide a database of 169 TNOs with high-precision dynamical classification and known discovery efficiency. Using this database, we find that the classical belt is a complex region with sub-structures that go beyond the usual splitting of inner (interior to 3:2 mean-motion resonance [MMR]), main (between 3:2 and 2:1 MMR), and outer (exterior to 2:1 MMR). The main classical belt (a = 40–47 AU) needs to be modeled with at least three components: the “hot” component with a wide inclination distribution and two “cold” components (stirred and kernel) with much narrower inclination distributions. The hot component must have a significantly shallower absolute magnitude (Hg) distribution than the other two components. With 95% confidence, there are 8000 +18001600 objects in the main belt with Hg 8.0, of which 50% are from the hot component, 40% from the stirred component, and 10% from the kernel; the hot component’s fraction drops rapidly with increasing Hg. Because of this, the apparent population fractions depend on the depth and ecliptic latitude of a trans-Neptunian survey. The stirred and kernel components are limited to only a portion of the main belt, while we find that the hot component is consistent with a smooth extension throughout the inner, main, and outer regions of the classical belt; in fact, the inner and outer belts are consistent with containing only hot-component objects. The Hg 8.0 TNO population estimates are 400 for the inner belt and 10,000 for the outer belt to within a factor of two (95% confidence). We show how the CFEPS Survey Simulator can be used to compare a cosmogonic model for the orbital element distribution to the real Kuiper Belt.
The Astrophysical Journal | 2013
P. Rousselot; O. Pirali; Emmanuel Jehin; Michel Vervloet; Damien Hutsemekers; Jean Manfroid; Daniel Cordier; Marie-Aline Martin-Drumel; Sébastien Gruet; Claude Arpigny; Alice Decock; Olivier Mousis
Determination of the nitrogen isotopic ratios in different bodies of the solar system provides important information regarding the solar systems origin. We unambiguously identified emission lines in comets due to the 15NH2 radical produced by the photodissociation of 15NH3. Analysis of our data has permitted us to measure the 14N/15N isotopic ratio in comets for a molecule carrying the amine (-NH) functional group. This ratio, within the error, appears similar to that measured in comets in the HCN molecule and the CN radical, and lower than the protosolar value, suggesting that N2 and NH3 result from the separation of nitrogen into two distinct reservoirs in the solar nebula. This ratio also appears similar to that measured in Titans atmospheric N2, supporting the hypothesis that, if the latter is representative of its primordial value in NH3, these bodies were assembled from building blocks sharing a common formation location.
Nature | 2004
Matthew J. Holman; J. J. Kavelaars; Tommy Grav; Brett James Gladman; Wesley Christopher Fraser; Dan Milisavljevic; Philip D. Nicholson; Joseph A. Burns; Valerio Carruba; Jean-Marc Petit; P. Rousselot; Oliver Mousis; Brian G. Marsden; Robert A. Jacobson
Each giant planet of the Solar System has two main types of moons. ‘Regular’ moons are typically larger satellites with prograde, nearly circular orbits in the equatorial plane of their host planets at distances of several to tens of planetary radii. The ‘irregular’ satellites (which are typically smaller) have larger orbits with significant eccentricities and inclinations. Despite these common features, Neptunes irregular satellite system, hitherto thought to consist of Triton and Nereid, has appeared unusual. Triton is as large as Pluto and is postulated to have been captured from heliocentric orbit; it traces a circular but retrograde orbit at 14 planetary radii from Neptune. Nereid, which exhibits one of the largest satellite eccentricities, is believed to have been scattered from a regular satellite orbit to its present orbit during Tritons capture. Here we report the discovery of five irregular moons of Neptune, two with prograde and three with retrograde orbits. These exceedingly faint (apparent red magnitude mR = 24.2–25.4) moons, with diameters of 30 to 50 km, were presumably captured by Neptune.
The Astrophysical Journal | 2009
Brett James Gladman; J. Kavelaars; J.-M. Petit; M. L. N. Ashby; Joel Wm. Parker; Jaime Coffey; Roger Jones; P. Rousselot; Olivier Mousis
We report the discovery of the first transneptunian object known to be on a retrograde orbit. The discovery was made during an outer solar system survey using the Canada–France–Hawaii Telescope (CFHT). After recovery observations on the MMT, CTIO-Blanco, Gemini-South, and CFHT telescopes, we can state with certainty that the object is both transneptunian and orbits the Sun in a retrograde sense, with an orbital inclination i = 104 deg. The object has IAU Minor Planet Center provisional designation 2008 KV42 and temporary nickname “Drac.” Numerical integration of a set of initial states consistent with the astrometry shows that the semimajor axis is a � 42 AU, the perihelion distance is q ∼21 AU, and that the object’s orbit evolves on ∼30 million year timescales via gravitational encounters with Uranus and Neptune. The object is unlikely to be primordial and thus needs a supply mechanism from a long-lived source. We outline several scenarios which could have emplaced the object on its current orbit, including a currently unobserved reservoir of large-inclination orbits beyond Neptune which may also supply the Halley-type comets.
Science | 2008
J.-M. Petit; J. J. Kavelaars; Brett James Gladman; Jean-Luc Margot; P. D. Nicholson; Roger Jones; J. Wm. Parker; Matthew L. N. Ashby; A. Campo Bagatin; Paula Gabriela Benavídez; Jaime Coffey; P. Rousselot; Olivier Mousis; Patrick A. Taylor
The study of binary Kuiper Belt objects helps to probe the dynamic conditions present during planet formation in the solar system. We report on the mutual-orbit determination of 2001 QW322, a Kuiper Belt binary with a very large separation whose properties challenge binary-formation and -evolution theories. Six years of tracking indicate that the binarys mutual-orbit period is ≈25 to 30 years, that the orbit pole is retrograde and inclined 50° to 62° from the ecliptic plane, and, most surprisingly, that the mutual orbital eccentricity is <0.4. The semimajor axis of 105,000 to 135,000 kilometers is 10 times that of other near-equal-mass binaries. Because this weakly bound binary is prone to orbital disruption by interlopers, its lifetime in its present state is probably less than 1 billion years.
The Astronomical Journal | 2011
P. Rousselot; Emmanuel Jehin; Jean Manfroid; Olivier Mousis; Christophe Dumas; B. Carry; U. Marboeuf; J.-M. Zucconi
There are hints that the dwarf planet (1) Ceres may contain a large amount of water ice. Some models and previous observations suggest that ice could be close enough to the surface to create a flux of water outward through the regolith. This work aims to confirm a previous detection of OH emission off the northern limb of Ceres with the International Ultraviolet Explorer (IUE). Such emission would be evidence of water molecules escaping from the dwarf planet. We used the Ultraviolet and Visual Echelle Spectrograph of the Very Large Telescope to obtain spectra off the northern and southern limbs of Ceres at several epochs. These spectra cover the 307-312 nm wavelength range corresponding to the OH (0,0) emission band, which is the brightest band of this radical, well known in the cometary spectra. These new observations, five times more sensitive than those from IUE, did not permit detection of OH around Ceres. We derive an upper limit for the water production of about {approx}7 x 10{sup 25} molecules s{sup -1} and estimate the minimum thickness of the dust surface layer above the water ice layer (if present) to be about 20 m.
Experimental Astronomy | 2014
Olivier Mousis; R. Hueso; J.-P. Beaulieu; Sylvain Bouley; B. Carry; F. Colas; A. Klotz; C. Pellier; J.-M. Petit; P. Rousselot; Mohamad Ali-Dib; W. Beisker; M. Birlan; C. Buil; A. Delsanti; E. Frappa; Heidi B. Hammel; Anny Chantal Levasseur-Regourd; Glenn S. Orton; A. Sánchez-Lavega; A. Santerne; P. Tanga; J. Vaubaillon; B. Zanda; David Baratoux; T. Böhm; V. Boudon; A. Bouquet; L. Buzzi; J. L. Dauvergne
Amateur contributions to professional publications have increased exponentially over the last decades in the field of planetary astronomy. Here we review the different domains of the field in which collaborations between professional and amateur astronomers are effective and regularly lead to scientific publications.We discuss the instruments, detectors, software and methodologies typically used by amateur astronomers to collect the scientific data in the different domains of interest. Amateur contributions to the monitoring of planets and interplanetary matter, characterization of asteroids and comets, as well as the determination of the physical properties of Kuiper Belt Objects and exoplanets are discussed.
The Astronomical Journal | 2016
Michele T. Bannister; J. J. Kavelaars; Jean-Marc Petit; Brett James Gladman; Stephen Gwyn; Ying-Tung Chen; Kathryn Volk; Mike Alexandersen; Susan D. Benecchi; A. Delsanti; Wesley C. Fraser; Mikael Granvik; William M. Grundy; A. Guilbert-Lepoutre; Daniel Hestroffer; Wing-Huen Ip; Marian Jakubik; R. Lynne Jones; Nathan A. Kaib; Catherine F. Kavelaars; Pedro Lacerda; S. M. Lawler; M. J. Lehner; Hsing-Wen Lin; Tim Lister; Patryk Sofia Lykawka; Stephanie Monty; Michael Marsset; Ruth A. Murray-Clay; Keith S. Noll
National Research Council of Canada; National Science and Engineering Research Council of Canada; Academia Sinica Postdoctoral Fellowship
Planetary and Space Science | 2014
Olivier Mousis; Leigh N. Fletcher; J. P Lebreton; Peter Wurz; T. Cavalié; Athena Coustenis; R Courtin; Daniel Gautier; Ravit Helled; P. G. J. Irwin; A. D. Morse; N. Nettelmann; Bernard Marty; P. Rousselot; Olivia Venot; D. H. Atkinson; J. H. Waite; K. Reh; Amy A. Simon; Sushil K. Atreya; N. André; Michel Blanc; Ioannis A. Daglis; G. Fischer; W. D Geppertt; Tristan Guillot; Matthew Mckay Hedman; R. Hueso; E. Lellouch; Jonathan I. Lunine
Remote sensing observations meet some limitations when used to study the bulk atmospheric composition of the giant planets of our solar system. A remarkable example of the superiority of in situ probe measurements is illustrated by the exploration of Jupiter, where key measurements such as the determination of the noble gases׳ abundances and the precise measurement of the helium mixing ratio have only been made available through in situ measurements by the Galileo probe. This paper describes the main scientific goals to be addressed by the future in situ exploration of Saturn placing the Galileo probe exploration of Jupiter in a broader context and before the future probe exploration of the more remote ice giants. In situ exploration of Saturn׳s atmosphere addresses two broad themes that are discussed throughout this paper: first, the formation history of our solar system and second, the processes at play in planetary atmospheres. In this context, we detail the reasons why measurements of Saturn׳s bulk elemental and isotopic composition would place important constraints on the volatile reservoirs in the protosolar nebula. We also show that the in situ measurement of CO (or any other disequilibrium species that is depleted by reaction with water) in Saturn׳s upper troposphere may help constraining its bulk O/H ratio. We compare predictions of Jupiter and Saturn׳s bulk compositions from different formation scenarios, and highlight the key measurements required to distinguish competing theories to shed light on giant planet formation as a common process in planetary systems with potential applications to most extrasolar systems. In situ measurements of Saturn׳s stratospheric and tropospheric dynamics, chemistry and cloud-forming processes will provide access to phenomena unreachable to remote sensing studies. Different mission architectures are envisaged, which would benefit from strong international collaborations, all based on an entry probe that would descend through Saturn׳s stratosphere and troposphere under parachute down to a minimum of 10 bar of atmospheric pressure. We finally discuss the science payload required on a Saturn probe to match the measurement requirements.
Astrobiology | 2015
Olivier Mousis; Eric Chassefière; Nils G. Holm; Alexis Bouquet; J. H. Waite; Wolf D. Geppert; S. Picaud; Yuri Aikawa; Mohamad Ali-Dib; Jean-Luc Charlou; P. Rousselot
We review the reservoirs of methane clathrates that may exist in the different bodies of the Solar System. Methane was formed in the interstellar medium prior to having been embedded in the protosolar nebula gas phase. This molecule was subsequently trapped in clathrates that formed from crystalline water ice during the cooling of the disk and incorporated in this form into the building blocks of comets, icy bodies, and giant planets. Methane clathrates may play an important role in the evolution of planetary atmospheres. On Earth, the production of methane in clathrates is essentially biological, and these compounds are mostly found in permafrost regions or in the sediments of continental shelves. On Mars, methane would more likely derive from hydrothermal reactions with olivine-rich material. If they do exist, martian methane clathrates would be stable only at depth in the cryosphere and sporadically release some methane into the atmosphere via mechanisms that remain to be determined. In the case of Titan, most of its methane probably originates from the protosolar nebula, where it would have been trapped in the clathrates agglomerated by the satellites building blocks. Methane clathrates are still believed to play an important role in the present state of Titan. Their presence is invoked in the satellites subsurface as a means of replenishing its atmosphere with methane via outgassing episodes. The internal oceans of Enceladus and Europa also provide appropriate thermodynamic conditions that allow formation of methane clathrates. In turn, these clathrates might influence the composition of these liquid reservoirs. Finally, comets and Kuiper Belt Objects might have formed from the agglomeration of clathrates and pure ices in the nebula. The methane observed in comets would then result from the destabilization of clathrate layers in the nuclei concurrent with their approach to perihelion. Thermodynamic equilibrium calculations show that methane-rich clathrate layers may exist on Pluto as well. Key Words: Methane clathrate-Protosolar nebula-Terrestrial planets-Outer Solar System. Astrobiology 15, 308-326.