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TOPIC: Extrasolar Planets


L

Posts: 131433
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RE: Extrasolar Planets
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Astronomers have discovered what may be the smallest alien planet yet a rocky "super-Earth" only four times heavier than our home planet.
It's orbiting a small star at a distance that puts it in the so-called "habitable zone" a region neither too hot nor too cold for liquid water and therefore suitable for possible life.
Scientists believe such Earth-like planets are the best hope for detecting evidence of living organisms beyond our solar system.
The tentative finding, which has yet to be confirmed, was reported during the May meeting of the International Astronomical Union in Cambridge, Mass.

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COROT-exo-3b
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Two new exoplanets and an unknown celestial object are the latest findings of the COROT mission. These discoveries mean that the mission has now found a total of four new exoplanets.
These results were presented this week at the IAU symposium 253 in Massachusetts, USA.

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RE: Extrasolar Planets
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Title: Microlensing Detections of Moons of Exoplanets
Authors: Cheongho Han

We investigate the characteristic of microlensing signals of Earth-like moons orbiting ice-giant planets. From this, we find that non-negligible satellite signals occur when the planet-moon separation is similar to or greater than the Einstein radius of the planet. We find that the satellite signal does not diminish with the increase of the planet-moon separation beyond the Einstein radius of the planet unlike the planetary signal which vanishes when the planet is located well beyond the Einstein radius of the star. We also find that the satellite signal tends to have the same sign as that of the planetary signal. These tendencies are caused by the lensing effect of the star on the moon in addition to the effect of the planet. We determine the range of satellite separations where the microlensing technique is optimised for the detections of moons. By setting an upper limit as the angle-average of the projected Hill radius and a lower limit as the half of the Einstein radius of the planet, we find that the microlensing method would be sensitive to moons with projected separations from the planet of 0.05 AU <~ d_ p <~0.24 AU for a Jupiter-mass planet, 0.03 AU <~ d_p <~ 0.17 AU for a Saturn-mass planet, and 0.01 AU <~ d_ p <~ 0.08 AU for a Uranus-mass planet. We compare the characteristics of the moons to be detected by the microlensing and transit techniques.

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Title: XO-4b: An Extrasolar Planet Transiting an F5V Star
Authors: P. R. McCullough, Christopher J. Burke, Jeff A. Valenti, Doug Long, Christopher M. Johns-Krull, P. Machalek, K. A. Janes, B. Taylor, J. Gregorio, C. N. Foote, Bruce L. Gary, M. Fleenor, Enrique García-Melendo, T. Vanmunster

We report the discovery of the planet XO-4b, which transits the star XO-4 (GSC 03793-01994, V=10.7, F5V). Transits are 1.0% deep and 4.4 hours in duration. The star XO-4 has a mass of 1.32 M_sun.... The planet XO-4b has a mass of 1.72 M_Jup....radius of 1.34 R_Jup...orbital period 4.125 days. We analyse scintillation-limited differential R-band photometry of XO-4b in transit made with a 1.8-m telescope under photometric conditions, yielding photometric precision of 0.6 to 2.0 millimag per one-minute interval. The declination of XO-4 places it within the continuous viewing zone of the Hubble Space Telescope (HST), which permits observation without interruption caused by occultation by the Earth. Because the stellar rotation periods of the three hottest stars orbited by transiting gas-giant planets are 2.0, 1.1, and 2.0 times the planetary orbital periods, we note the possibility of resonant interaction.

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Title: XO-5b: A Transiting Jupiter-sized Planet With A Four Day Period
Authors: Christopher J. Burke, P. R. McCullough, Jeff A. Valenti, Doug Long, Christopher M. Johns-Krull, P. Machalek, Kenneth A. Janes, B. Taylor, Michael L. Fleenor, Cindy N. Foote, Bruce L. Gary, Enrique Garcia-Melendo, J. Gregorio, T. Vanmunster

The star XO-5 (GSC 02959-00729, V=12.1, G8V) hosts a Jupiter-sized, Rp=1.15±0.12 Rjup, transiting extrasolar planet, XO-5b, with an orbital period of P=4.187732±0.00002 days. The planet mass (Mp=1.15±0.08 Mjup) and surface gravity (gp=22±5 m/s^2) are significantly larger than expected by empirical Mp-P and Mp-P-[Fe/H] relationships. However, the deviation from the Mp-P relationship for XO-5b is not large enough to suggest a distinct type of planet as is suggested for GJ 436b, HAT-P-2b, and XO-3b. By coincidence XO-5 overlies the extreme H I plume that emanates from the interacting galaxy pair NGC 2444/NGC 2445 (Arp 143).

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Title: Theoretical Radii of Extrasolar Giant Planets: the Cases of TrES-4, XO-3b, and HAT-P-1b
Authors: Xin Liu, Adam Burrows, Laurent Ibgui

To explain their observed radii, we present theoretical radius-age trajectories for the extrasolar giant planets (EGPs) TrES-4, XO-3b, and HAT-P-1b. We factor in variations in atmospheric opacity, the presence of an inner heavy-element core, and possible heating due to orbital tidal dissipation. A small, yet non-zero, degree of core heating is needed to explain the observed radius of TrES-4, unless its atmospheric opacity is significantly larger than a value equivalent to that at 10 x solar metallicity with equilibrium molecular abundances. This heating rate is reasonable, and corresponds for an energy dissipation parameter (Q_p) of  ~10^5 to an eccentricity of  ~0.04, assuming 3 x solar atmospheric opacity. For XO-3b, which has an observed orbital eccentricity of 0.26, we show that tidal heating needs to be taken into account to explain its observed radius. Furthermore, we re-examine the core mass needed for HAT-P-1b in light of new measurements and find that it now generally follows the correlation between stellar metallicity and core mass suggested by burrows07b. Given various core heating rates, theoretical grids and fitting formulae for a giant planet's equilibrium radius and equilibration timescale are provided for planet masses M_p= 0.5, 1.0, and 1.5 M_J with a = 0.02-0.06 AU, orbiting a G2V star. When the equilibration timescale is much shorter than that of tidal heating variation, the "effective age" of the planet is shortened, resulting in evolutionary trajectories more like those of younger EGPs. Motivated by the work of  jackson08a,jackson08b, we suggest that this "clock-reset" effect could indeed be important in better explaining some observed transit radii.

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Title: Disk Dispersal and Planet Formation Time Scales
Authors: Lynne A. Hillenbrand

Well before the existence of exo-solar systems was confirmed, it was accepted knowledge that most -- if not all -- stars possess circumstellar material during the first one-to-several million years of their pre-main sequence lives, and thus that they commonly have the potential to form planets. Here I summarize current understanding regarding the evolution of proto-planetary dust and gas disks, emphasizing the diversity in evolutionary paths.

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Title: Planetary Systems in Binaries. I. Dynamical Classification
Authors: Genya Takeda, Ryosuke Kita, Frederic A. Rasio (Northwestern Univ.)
(Version v2)

Many recent observational studies have concluded that planetary systems commonly exist in multiple-star systems. At least ~20% of the known extrasolar planetary systems are associated with one or more stellar companions. The orbits of stellar binaries hosting planetary systems are typically wider than 100 AU and often highly inclined with respect to the planetary orbits. The effect of secular perturbations from such an inclined binary orbit on a coupled system of planets, however, is little understood theoretically. In this paper we investigate various dynamical classes of double-planet systems in binaries through numerical integrations and we provide an analytic framework based on secular perturbation theories. Differential nodal precession of the planets is the key property that separates two distinct dynamical classes of multiple planets in binaries: (1) dynamically-rigid systems in which the orbital planes of planets precess in concert as if they were embedded in a rigid disk, and (2) weakly-coupled systems in which the mutual inclination angle between initially coplanar planets grows to large values on secular timescales. In the latter case, the quadrupole perturbation from the outer planet induces additional Kozai cycles and causes the orbital eccentricity of the inner planet to oscillate with large amplitudes. The cyclic angular momentum transfer from a stellar companion propagating inward through planets can significantly alter the orbital properties of the inner planet on shorter timescales. This perturbation propagation mechanism may offer important constraints on the presence of additional planets in known single-planet systems in binaries.

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HD 75289Ab
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Title: HD 75289Ab revisited - Searching for starlight reflected from a hot Jupiter
Authors: F. Rodler, M. Kuerster, T. Henning

Aims. We attempt to detect starlight reflected from a hot Jupiter, orbiting the main-sequence star HD 75289Ab. We report a revised analysis of observations of this planetary system presented previously by another research group.
    Methods. We analyse high-precision, high-resolution spectra, collected over four nights using UVES at the VLT/UT2, by way of data synthesis. We try to interpret our data using different atmospheric models for hot Jupiters.
    Results. We do not find any evidence for reflected light, and, therefore, establish revised upper limits to the planet-to-star flux ratio at the 99.9% significance level. At high orbital inclinations, where the best sensitivity is attained, we can limit the relative reflected radiation to be less than e = 6.7 x 10-5 assuming a grey albedo, and e = 8.3 x 10-5 assuming an Class IV function, respectively. This implies a geometric albedo smaller than p = 0.46 and p = 0.57, for the grey albedo and the Class IV albedo shape, respectively, assuming a planetary radius of 1.2 RJup.

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RE: Extrasolar Planets
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Title: Limits to the planet candidate GJ 436c
Authors: R. Alonso (1), M. Barbieri (1), M. Rabus (2), H.J. Deeg (2), J.A. Belmonte (2), J.M. Almenara (2) ((1) LAM, France, (2) IAC, Spain)
 
We report on H-band ground-based observations of a transit of the hot Neptune GJ 436b. Once combined to achieve an equivalent sampling as archived observations taken with Spitzer, our measurements reach comparable precision levels. We analyse both sets of observations in a consistent way, and measure the rate of orbital inclination change to be of 0.02+/-0.04 degrees in the time span between the two observations (253.8 d, corresponding to 0.03+/-0.05 degrees/yr if extrapolated). By performing simulations of planetary systems including a second planet GJ 436c which has been recently suggested (Ribas et al. 2008), this rate allows to put limits to the relative inclination between the two planets. The allowed inclinations for a 5 M_E super-Earth GJ 436c in a 5.2 d orbit are within ~7 degrees of the one of GJ 436b; for larger differences the observed inclination change can be reproduced only during short sections (<50%) of the orbital evolution of the system. The measured times of three transit centres of the system do not show any departure from linear ephemeris, a result that is only reproduced in <1% of the simulated orbits. Put together, these results argue against the proposed planet candidate GJ 436c.

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