THE 8 μm PHASE VARIATION OF THE HOT SATURN HD 149026b

被引:107
|
作者
Knutson, Heather A. [1 ]
Charbonneau, David [1 ]
Cowan, Nicolas B. [2 ]
Fortney, Jonathan J. [3 ]
Showman, Adam P. [4 ,5 ]
Agol, Eric [2 ]
Henry, Gregory W. [6 ]
机构
[1] Harvard Smithsonian Ctr Astrophys, Cambridge, MA 02138 USA
[2] Univ Washington, Dept Astron, Seattle, WA 98195 USA
[3] Univ Calif Santa Cruz, Univ Calif Observ, Lick Observ, Dept Astron & Astrophys, Santa Cruz, CA 95064 USA
[4] Univ Arizona, Lunar & Planetary Lab, Tucson, AZ 85721 USA
[5] Univ Arizona, Dept Planetary Sci, Tucson, AZ 85721 USA
[6] Tennessee State Univ, Ctr Excellence Informat Syst, Nashville, TN 37209 USA
基金
美国国家科学基金会;
关键词
eclipses; planetary systems; stars: individual (HD 149026b); techniques: photometric; INFRARED-EMISSION SPECTRUM; EXTRASOLAR GIANT PLANETS; LIGHT-CURVE PROJECT; ATMOSPHERIC CIRCULATION; TRANSIT PHOTOMETRY; THERMAL EMISSION; ROTATION PERIOD; JUPITERS; MASS; TEMPERATURE;
D O I
10.1088/0004-637X/703/1/769
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We monitor the star HD 149026 and its Saturn-mass planet at 8.0 mu m over slightly more than half an orbit using the Infrared Array Camera on the Spitzer Space Telescope. We find an increase of 0.0227% +/- 0.0066% (3.4 sigma significance) in the combined planet-star flux during this interval. The minimum flux from the planet is 45% +/- 19% of the maximum planet flux, corresponding to a difference in brightness temperature of 480 +/- 140 K between the two hemispheres. We derive a new secondary eclipse depth of 0.0411% +/- 0.0076% in this band, corresponding to a dayside brightness temperature of 1440 +/- 150 K. Our new secondary eclipse depth is half that of a previous measurement (3.0 sigma difference) in this same bandpass by Harrrington et al. We re-fit the Harrrington et al. data and obtain a comparably good fit with a smaller eclipse depth that is consistent with our new value. In contrast to earlier claims, our new eclipse depth suggests that this planet's dayside emission spectrum is relatively cool, with an 8 mu m brightness temperature that is less than the maximum planet-wide equilibrium temperature. We measure the interval between the transit and secondary eclipse and find that that the secondary eclipse occurs 20.9(-6.5)(+7.2) minutes earlier (2.9 sigma) than predicted for a circular orbit, a marginally significant result. This corresponds to e cos (omega) = -0.0079(-0.0025)(+0.0027), where e is the planet's orbital eccentricity and omega is the argument of pericenter.
引用
收藏
页码:769 / 784
页数:16
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