2011ApJS..197....1M


Query : 2011ApJS..197....1M

2011ApJS..197....1M - Astrophys. J., Suppl. Ser., 197, 1 (2011/November-0)

The distribution of transit durations for Kepler planet candidates and implications for their orbital eccentricities.

MOORHEAD A.V., FORD E.B., MOREHEAD R.C., ROWE J., BORUCKI W.J., BATALHA N.M., BRYSON S.T., CALDWELL D.A., FABRYCKY D.C., GAUTIER T.N., KOCH D.G., HOLMAN M.J., JENKINS J.M., LI J., LISSAUER J.J., LUCAS P., MARCY G.W., QUINN S.N., QUINTANA E., RAGOZZINE D., SHPORER A., STILL M. and TORRES G.

Abstract (from CDS):

Doppler planet searches have discovered that giant planets follow orbits with a wide range of orbital eccentricities, revolutionizing theories of planet formation. The discovery of hundreds of exoplanet candidates by NASA's Kepler mission enables astronomers to characterize the eccentricity distribution of small exoplanets. Measuring the eccentricity of individual planets is only practical in favorable cases that are amenable to complementary techniques (e.g., radial velocities, transit timing variations, occultation photometry). Yet even in the absence of individual eccentricities, it is possible to study the distribution of eccentricities based on the distribution of transit durations (relative to the maximum transit duration for a circular orbit). We analyze the transit duration distribution of Kepler planet candidates. We find that for host stars with Teff> 5100 K we cannot invert this to infer the eccentricity distribution at this time due to uncertainties and possible systematics in the host star densities. With this limitation in mind, we compare the observed transit duration distribution with models to rule out extreme distributions. If we assume a Rayleigh eccentricity distribution for Kepler planet candidates, then we find best fits with a mean eccentricity of 0.1-0.25 for host stars with Teff≤ 5100 K. We compare the transit duration distribution for different subsets of Kepler planet candidates and discuss tentative trends with planetary radius and multiplicity. High-precision spectroscopic follow-up observations for a large sample of host stars will be required to confirm which trends are real and which are the results of systematic errors in stellar radii. Finally, we identify planet candidates that must be eccentric or have a significantly underestimated stellar radius.

Abstract Copyright: ∼

Journal keyword(s): planets and satellites: fundamental parameters

Simbad objects: 16

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Number of rows : 16
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 Kepler-9b Pl 19 02 17.7544327200 +38 24 03.176851896           ~ 121 1
2 Kepler-9c Pl 19 02 17.7544327200 +38 24 03.176851896           ~ 109 1
3 Kepler-12 Er* 19 04 58.4220633696 +50 02 25.271762064   13.96   13.68   G0 97 1
4 Kepler-238 Er* 19 11 35.3058296736 +40 38 16.143812448       15.189   ~ 77 0
5 Kepler-117 Er* 19 15 10.3301577216 +48 02 24.785162160   15.056 14.476 14.266 13.69 F2 94 1
6 Kepler-428 Ro* 19 22 19.6164487104 +40 34 38.564097492   16.584 15.405 15.101 14.84 K1V 50 0
7 Kepler-503 Ro* 19 22 32.7571535424 +38 42 27.580385304           ~ 45 0
8 Kepler-435 Er* 19 29 08.9490159624 +43 11 50.159878764   14.228 13.772 13.665 12.92 F5V 77 1
9 Kepler-108 ** 19 38 14.20056 +46 03 44.3700       12.485   ~ 103 0
10 Kepler-678 Ro* 19 41 49.2709626072 +50 29 40.371017892           ~ 38 0
11 Kepler-719 * 19 42 08.6609695800 +43 53 04.012955376           ~ 26 0
12 KOI-51 EB* 19 43 40.4235051432 +41 19 55.393696740           ~ 30 1
13 Kepler-731 EB* 19 45 34.3632953784 +45 34 06.816377604           ~ 41 0
14 Kepler-40 Ro* 19 47 15.2874297936 +47 31 35.665322736   15.11   14.89 14.02 F5IV 55 1
15 Kepler-494 Ro* 19 48 51.3750498576 +41 39 50.524488036           ~ 41 0
16 Kepler-433 EB* 19 50 22.4722397592 +40 58 38.154033120   15.373 14.574 14.81 14.10 ~ 57 1

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