text
stringlengths 0
44.4k
|
---|
shorter for hotter planets, but the temperature-dependance of the radiative timescale is stronger, |
leading to decreased heat recirculation efficiency. |
Subject headings: methods: data analysis — (stars:) planetary systems — |
1.INTRODUCTION |
Short-period exoplanets are expected to have atmo- |
spheric compositions and dynamics that differ signifi- |
cantly from Solar System giant planets3. These planets |
orbit∼100×closer to their host stars than Jupiter does |
from the Sun. As a result, they receive ∼104×more flux |
andexperiencetidalforces ∼106×strongerthanJupiter. |
In contrast to Jupiter, which releases roughly as much |
power in its interior as it receives from the Sun, short- |
period exoplanets have power budgets dictated by the |
flux they receive from their host stars. Roughly speak- |
ing, the stellar flux incident on a planet does one of two |
things: it is reflected back into space, or advected else- |
where on the planet and re-radiated at different wave- |
lengths. The physical parameters that describe these |
processes are the planet’s Bond albedo and redistribu- |
tion efficiency. |
1.1.Albedo |
1CIERA Fellow, Northwestern University, 2131 Tech Dr, |
Evanston, IL 60208 |
email: n-cowan@northwestern.edu |
2Astronomy Department, University of Washington, Box |
351580, Seattle, WA 98195 |
3For our purposes a “short period” exoplanet is one where the |
periastron distance is less than 0 .1 AU, regardless of its actual |
period, and regardless of mass, which may range from Neptune - |
sized to Brown Dwarf. They are all Class IV and V extrasolar |
giant planets in the scheme of Sudarsky et al. (2003).Giant planets in the Solar System have albedos greater |
than 50%because ofthe presenceofcondensedmolecules |
(H2O, CH 4, NH3, etc.) in their atmospheres. Planets |
with effective temperatures exceeding ∼400 K should be |
cloud free, leading to albedos of 0.05–0.4 (Marley et al. |
1999). If pressure-broadenedNa and K opacity is impor- |
tant at optical wavelengths (as it is for brown dwarfs, |
Burrows et al. 2000), then the Bond albedos of hot |
Jupiters may be less than 10% (Sudarsky et al. 2000). |
But the very hottest planets, the so-called class V extra- |
solar giant planets ( Teff>1500 K), might have very high |
albedosdue to a high silicate cloud layer(Sudarsky et al. |
2000). For a planet whose albedo is dominated by |
clouds (as opposed to Rayleigh scattering) the albedo |
depends on the composition and size of cloud particles |
(Seager et al. 2000). |
Earlyattempts to observe reflected light from exoplan- |
ets (Charbonneau et al. 1999; Collier Cameron et al. |
2002a; Leigh et al. 2003a,b; Rodler et al. 2008, 2010) in- |
dicated that they might not be as reflective as Solar Sys- |
tem gas giants (for a review, see Langford et al. 2010). |
Measurements of HD 209458b taken with the Cana- |
dian MOST satellite revealed a very low albedo ( <8%, |
Rowe et al.2008), andit hassincebeentakenforgranted |
that all short-period planets have albedos on par with |
that of charcoal. |
From the standpoint of the planet’s climate, the im- |
portant factor is not the albedo at any one wavelength,2 Cowan & Agol |
Aλ, but rather the integrated albedo, weighted by the in- |
cident stellar spectrum, known as the Bond albedo and |
denoted in this paper as AB. The relation between Aλ |
and the planet’s Bond albedo is not trivial. If the albedo |
is dominated by gray clouds, then the albedo at a sin- |
gle wavelength can indeed be extrapolated to obtain AB. |
For non-grayreflectance spectra, however, it is critical to |
measureAλat the peak emitting wavelength of the host |
startoobtainagoodestimateofthe planet’senergybud- |
get. For example, as pointed out in Marley et al. (1999), |
planets with identical albedo spectra, Aλ, mayhaveradi- |
cally different ABdepending on the spectraltype oftheir |
host stars. |
1.2.Redistribution Efficiency |
The first few measurements of hot Jupiter phase vari- |
ations showed signs that these planets are not all cut |
from the same cloth. Harrington et al. (2006) and |
Knutson et al. (2007a) quoted very different phase func- |
tion amplitudes for the υAndromeda and HD 189733 |
systems. It was not clear whether the differences were |
intrinsic to the planets, however, because the data |
were taken with different instruments, at different wave- |
lengths, and with very different observation schemes (in |
any case, subsequent re-analysis of the original data and |
newly aquired Spitzerobservations of υAndromeda b |
paint a completely different picture of that system: |
Crossfield et al. 2010). |
The uniform study presented in Cowan et al. (2007), |
on the other hand, showed that HD 179949b and |
HD209458bexhibit significantlydifferentdegreesofheat |
recirculation, confirming suspicions. But it was not clear |
whether hot exoplanets were uni-modal or bi-modal in |
redistribution: are HD 179949b and HD 209458b end- |
members of a single distribution, or prototypes for two |
fundamentally different sorts of exoplanets? |
The presence or lack of a stratospheric tempera- |
ture inversion (Hubeny et al. 2003; Fortney et al. 2006; |
Burrows et al. 2007, 2008; Zahnle et al. 2009) on the |
day-sides of exoplanets has been invoked to explain |
a purported bi-modality in recirculation efficiency on |
hot Jupiters (Fortney et al. 2008). The argument, sim- |
ply put, is that optical absorbers high in the atmo- |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.