Clouds on the hot Jupiter HD189733b: constraints from the reflection spectrum

(2014)

Authors:

Joanna K Barstow, Suzanne Aigrain, Patrick GJ Irwin, Till Hackler, Leigh N Fletcher, Jae-Min Lee, Neale P Gibson

WTS-2 b: a hot Jupiter orbiting near its tidal destruction radius around a K dwarf

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 440:2 (2014) 1470-1489

Authors:

Jayne Birkby, M Cappetta, P Cruz, J Koppenhoefer, O Ivanyuk, Aj Mustill, St Hodgkin, Dj Pinfield, B Sipőcz, G Kovács, R Saglia, Y Pavlenko, D Barrado, A Bayo, D Campbell, S Catalan, L Fossati, M-C Gálvez-Ortiz, M Kenworthy, J Lillo-Box, El Martín, D Mislis, Ejw de Mooij, Sv Nefs, Iag Snellen, H Stoev, J Zendejas, C del Burgo, J Barnes, N Goulding, Ca Haswell, M Kuznetsov, N Lodieu, F Murgas, E Palle, E Solano, P Steele, R Tata

Abstract:

We report the discovery of WTS-2 b, an unusually close-in 1.02-d hot Jupiter (MP = 1.12MJ, RP = 1.30RJ) orbiting a K2V star, which has a possible gravitationally bound M-dwarf companion at 0.6 arcsec separation contributing ∼20 per cent of the total flux in the observed J-band light curve. The planet is only 1.5 times the separation from its host star at which it would be destroyed by Roche lobe overflow, and has a predicted remaining lifetime of just ∼40 Myr, assuming a tidal dissipation quality factor of Q′⋆=106⁠. Q′⋆ is a key factor in determining how frictional processes within a host star affect the orbital evolution of its companion giant planets, but it is currently poorly constrained by observations. We calculate that the orbital decay of WTS-2 b would correspond to a shift in its transit arrival time of Tshift ∼ 17 s after 15 yr assuming Q′⋆=106⁠. A shift less than this would place a direct observational constraint on the lower limit of Q′⋆ in this system. We also report a correction to the previously published expected Tshift for WASP-18 b, finding that Tshift = 356 s after 10 yr for Q′⋆=106⁠, which is much larger than the estimated 28 s quoted in WASP-18 b discovery paper. We attempted to constrain Q′⋆ via a study of the entire population of known transiting hot Jupiters, but our results were inconclusive, requiring a more detailed treatment of transit survey sensitivities at long periods. We conclude that the most informative and straightforward constraints on Q′⋆ will be obtained by direct observational measurements of the shift in transit arrival times in individual hot Jupiter systems. We show that this is achievable across the mass spectrum of exoplanet host stars within a decade, and will directly probe the effects of stellar interior structure on tidal dissipation.

Exploring the Diversity of Jupiter-Class Planets (Discussion Meeting Contribution)

(2014)

Authors:

Leigh N Fletcher, Patrick GJ Irwin, Joanna K Barstow, Remco J de Kok, Jae-Min Lee, Suzanne Aigrain

Neptune at summer solstice: Zonal mean temperatures from ground-based observations, 2003-2007

Icarus 231 (2014) 146-167

Authors:

LN Fletcher, I de Pater, GS Orton, HB Hammel, ML Sitko, PGJ Irwin

Abstract:

Imaging and spectroscopy of Neptune's thermal infrared emission from Keck/LWS (2003), Gemini-N/MICHELLE (2005); VLT/VISIR (2006) and Gemini-S/TReCS (2007) is used to assess seasonal changes in Neptune's zonal mean temperatures between Voyager-2 observations (1989, heliocentric longitude Ls=236°) and southern summer solstice (2005, Ls=270°). Our aim was to analyse imaging and spectroscopy from multiple different sources using a single self-consistent radiative-transfer model to assess the magnitude of seasonal variability. Globally-averaged stratospheric temperatures measured from methane emission tend towards a quasi-isothermal structure (158-164K) above the 0.1-mbar level, and are found to be consistent with spacecraft observations of AKARI. This remarkable consistency, despite very different observing conditions, suggests that stratospheric temporal variability, if present, is <±5K at 1mbar and <±3K at 0.1mbar during this solstice period. Conversely, ethane emission is highly variable, with abundance determinations varying by more than a factor of two (from 500 to 1200ppb at 1mbar). The retrieved C2H6 abundances are extremely sensitive to the details of the T(p) derivation, although the underlying cause of the variable ethane emission remains unidentified. Stratospheric temperatures and ethane are found to be latitudinally uniform away from the south pole (assuming a latitudinally-uniform distribution of stratospheric methane), with no large seasonal hemispheric asymmetries evident at solstice. At low and mid-latitudes, comparisons of synthetic Voyager-era images with solstice-era observations suggest that tropospheric zonal temperatures are unchanged since the Voyager 2 encounter, with cool mid-latitudes and a warm equator and pole. A re-analysis of Voyager/IRIS 25-50μm mapping of tropospheric temperatures and para-hydrogen disequilibrium (a tracer for vertical motions) suggests a symmetric meridional circulation with cold air rising at mid-latitudes (sub-equilibrium para-H2 conditions) and warm air sinking at the equator and poles (super-equilibrium para-H2 conditions). The most significant atmospheric changes have occurred at high southern latitudes, where zonal temperatures retrieved from 2003 images suggest a polar enhancement of 7-8K above the tropopause, and an increase of 5-6K throughout the 70-90°S region between 0.1 and 200mbar. Such a large perturbation, if present in 1989, would have been detectable by Voyager/IRIS in a single scan despite its long-wavelength sensitivity, and we conclude that Neptune's south polar cyclonic vortex increased in strength significantly from Voyager to solstice. © 2013 Elsevier Inc.

WTS-2 b: a hot Jupiter orbiting near its tidal destruction radius around a K-dwarf

(2014)

Authors:

JL Birkby, M Cappetta, P Cruz, J Koppenhoefer, O Ivanyuk, AJ Mustill, ST Hodgkin, DJ Pinfield, B Sipőcz, G Kovács, R Saglia, Y Pavlenko, D Barrado, A Bayo, D Campbell, S Catalan, L Fossati, M-C Gálvez-Ortiz, M Kenworthy, J Lillo-Box EL Martín, D Mislis, EJW de Mooij, SV Nefs, IAG Snellen, H Stoev, J Zendejas, C del Burgo, J Barnes, N Goulding, CA Haswell, M Kuznetsov, N Lodieu, F Murgas, E Palle, E Solano, P Steele, R Tata