Leslie A. Rogers
University of Chicago
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Featured researches published by Leslie A. Rogers.
Science | 2012
Joshua A. Carter; Eric Agol; W. J. Chaplin; Sarbani Basu; Timothy R. Bedding; Lars A. Buchhave; Jørgen Christensen-Dalsgaard; Katherine M. Deck; Y. Elsworth; Daniel C. Fabrycky; Eric B. Ford; Jonathan J. Fortney; S. J. Hale; R. Handberg; S. Hekker; Matthew J. Holman; Daniel Huber; Christopher Karoff; Steven D. Kawaler; Hans Kjeldsen; Jack J. Lissauer; Eric D. Lopez; Mikkel N. Lund; M. Lundkvist; T. S. Metcalfe; A. Miglio; Leslie A. Rogers; D. Stello; William J. Borucki; Steve Bryson
So Close and So Different In our solar system, the rocky planets have very distinct orbits from those of the gas giants. Carter et al. (p. 556, published online 21 June) report on a planetary system where this pattern does not apply, posing a challenge to theories of planet formation. Data from the Kepler space telescope reveal two planets with radically different densities orbiting the same star with very similar orbital periods. One planet has a rocky Earth-like composition and the other is akin to Neptune. The Kepler spacecraft detected a super-Earth and a Neptune-like planet in very tightly spaced orbits around the same star. In the solar system, the planets’ compositions vary with orbital distance, with rocky planets in close orbits and lower-density gas giants in wider orbits. The detection of close-in giant planets around other stars was the first clue that this pattern is not universal and that planets’ orbits can change substantially after their formation. Here, we report another violation of the orbit-composition pattern: two planets orbiting the same star with orbital distances differing by only 10% and densities differing by a factor of 8. One planet is likely a rocky “super-Earth,” whereas the other is more akin to Neptune. These planets are 20 times more closely spaced and have a larger density contrast than any adjacent pair of planets in the solar system.
Nature | 2012
Francois Fressin; Guillermo Torres; Jason F. Rowe; David Charbonneau; Leslie A. Rogers; Sarah Ballard; Natalie M. Batalha; William J. Borucki; Stephen T. Bryson; Lars A. Buchhave; David R. Ciardi; J.-M. Desert; Courtney D. Dressing; Daniel C. Fabrycky; Eric B. Ford; Thomas N. Gautier; Christopher E. Henze; Matthew J. Holman; Andrew W. Howard; Steve B. Howell; Jon M. Jenkins; David G. Koch; David W. Latham; Jack J. Lissauer; Geoffrey W. Marcy; Samuel N. Quinn; Darin Ragozzine; Dimitar D. Sasselov; Sara Seager; Fergal Mullally
Since the discovery of the first extrasolar giant planets around Sun-like stars, evolving observational capabilities have brought us closer to the detection of true Earth analogues. The size of an exoplanet can be determined when it periodically passes in front of (transits) its parent star, causing a decrease in starlight proportional to its radius. The smallest exoplanet hitherto discovered has a radius 1.42 times that of the Earth’s radius (R⊕), and hence has 2.9 times its volume. Here we report the discovery of two planets, one Earth-sized (1.03R⊕) and the other smaller than the Earth (0.87R⊕), orbiting the star Kepler-20, which is already known to host three other, larger, transiting planets. The gravitational pull of the new planets on the parent star is too small to measure with current instrumentation. We apply a statistical method to show that the likelihood of the planetary interpretation of the transit signals is more than three orders of magnitude larger than that of the alternative hypothesis that the signals result from an eclipsing binary star. Theoretical considerations imply that these planets are rocky, with a composition of iron and silicate. The outer planet could have developed a thick water vapour atmosphere.
The Astrophysical Journal | 2010
Leslie A. Rogers; Sara Seager
We present an analysis of the bulk composition of the MEarth transiting super-Earth exoplanet GJ 1214b using planet interior structure models. We consider three possible origins for the gas layer on GJ 1214b: direct accretion of gas from the protoplanetary nebula, sublimation of ices, and outgassing from rocky material. Armed only with measurements of the planet mass (Mp = 6.55 ± 0.98 M ⊕), radius (Rp = 2.678 ± 0.13 R ⊕), and stellar irradiation level, our main conclusion is that we cannot infer a unique composition. A diverse range of planet interiors fits the measured planet properties. Nonetheless, GJ 1214bs relatively low average density (ρ p = 1870 ± 400 kg m–3) means that it almost certainly has a significant gas component. Our second major conclusion is that under most conditions we consider GJ 1214b would not have liquid water. Even if the outer envelope is predominantly sublimated water ice, the envelope will likely consist of a super-fluid layer sandwiched between vapor above and plasma (electrically conductive fluid) below at greater depths. In our models, a low intrinsic planet luminosity (2TW) is needed for a water envelope on GJ 1214b to pass through the liquid phase.
The Astrophysical Journal | 2010
Leslie A. Rogers; Sara Seager
Several transiting super-Earths are expected to be discovered in the coming few years. While tools to model the interior structure of transiting planets exist, inferences about the composition are fraught with ambiguities. We present a framework to quantify how much we can robustly infer about super-Earth and Neptune-size exoplanet interiors from radius and mass measurements. We introduce quaternary diagrams to illustrate the range of possible interior compositions for planets with four layers (iron core, silicate mantles, water layers, and H/He envelopes). We apply our model to CoRoT-7b, GJ 436b, and HAT-P-11b. Interpretation of planets with H/He envelopes is limited by the model uncertainty in the interior temperature, while for CoRoT-7b observational uncertainties dominate. We further find that our planet interior model sharpens the observational constraints on CoRoT-7bs mass and radius, assuming the planet does not contain significant amounts of water or gas. We show that the strength of the limits that can be placed on a super-Earths composition depends on the planets density; for similar observational uncertainties, high-density super-Mercuries allow the tightest composition constraints. Finally, we describe how techniques from Bayesian statistics can be used to take into account in a formal way the combined contributions of both theoretical and observational uncertainties to ambiguities in a planets interior composition. On the whole, with only a mass and radius measurement an exact interior composition cannot be inferred for an exoplanet because the problem is highly underconstrained. Detailed quantitative ranges of plausible compositions, however, can be found.
The Astrophysical Journal | 2012
Thomas N. Gautier; David Charbonneau; Jason F. Rowe; Geoffrey W. Marcy; Howard Isaacson; Guillermo Torres; Francois Fressin; Leslie A. Rogers; J.-M. Desert; Lars A. Buchhave; David W. Latham; Samuel N. Quinn; David R. Ciardi; Daniel C. Fabrycky; Eric B. Ford; Ronald L. Gilliland; Lucianne M. Walkowicz; Stephen T. Bryson; William D. Cochran; Michael Endl; Debra A. Fischer; Steve B. Howell; Elliott P. Horch; Natalie M. Batalha; William J. Borucki; Jessie L. Christiansen; John C. Geary; Christopher E. Henze; Matthew J. Holman; Khadeejah A. Ibrahim
We present the discovery of the Kepler-20 planetary system, which we initially identified through the detection of five distinct periodic transit signals in the Kepler light curve of the host star 2MASSJ19104752+4220194. We find a stellar effective temperature T_(eff)=5455±100K, a metallicity of [Fe/H]=0.01±0.04, and a surface gravity of log(g)=4.4±0.1. Combined with an estimate of the stellar density from the transit light curves we deduce a stellar mass of M_*=0.912±0.034 M_⊙ and a stellar radius of R_*=0.944^(+0.060)_(-0.095) R_⊙. For three of the transit signals, our results strongly disfavor the possibility that these result from astrophysical false positives. We conclude that the planetary scenario is more likely than that of an astrophysical false positive by a factor of 2 x 10^5 (Kepler-20b), 1 x 10^5 (Kepler-20c), and 1.1 x 10^3 (Kepler-20d), sufficient to validate these objects as planetary companions. For Kepler-20c and Kepler-20d, the blend scenario is independently disfavored by the achromaticity of the transit: From Spitzer data gathered at 4.5µm, we infer a ratio of the planetary to stellar radii of 0.075±0.015 (Kepler-20c) and 0.065±0.011 (Kepler-20d), consistent with each of the depths measured in the Kepler optical bandpass. We determine the orbital periods and physical radii of the three confirmed planets to be 3.70d and 1.91^(+0.12)_(-0.21) R_⊕ for Kepler-20b, 10.85 d and 3.07^(+0.20)_(-0.31) R_⊕ for Kepelr-20c, and 77.61 d and 2.75^(+0.17)_(-0.30) R_⊕ for Kepler-20d. From multi-epoch radial velocities, we determine the masses of Kepler-20b and Kepler-20c to be 8.7±2.2 M_⊕ and 16.1±3.5 M_⊕, respectively, and we place an upper limit on the mass of Kepler-20d of 20.1 M_⊕ (2 σ).
The Astrophysical Journal | 2013
Ronald L. Gilliland; Geoffrey W. Marcy; Jason F. Rowe; Leslie A. Rogers; Guillermo Torres; Francois Fressin; Eric D. Lopez; Lars A. Buchhave; Jørgen Christensen-Dalsgaard; J.-M. Desert; Christopher E. Henze; Howard Isaacson; Jon M. Jenkins; Jack J. Lissauer; W. J. Chaplin; Sarbani Basu; T. S. Metcalfe; Y. Elsworth; R. Handberg; S. Hekker; Daniel Huber; C. Karoff; Hans Kjeldsen; Mikkel N. Lund; M. Lundkvist; A. Miglio; David Charbonneau; Eric B. Ford; Jonathan J. Fortney; Michael R. Haas
NASA’s Kepler Mission has revealed two transiting planets orbiting Kepler-68. Follow-up Doppler measurements have established the mass of the innermost planet and revealed a third Jovian-mass planet orbiting beyond the two transiting planets. Kepler-68b, in a 5.4 day orbit, has M_P = 8.3^(+2.2)_(−2.4) M_⊕, R_P = 2.31^(+0.06)_(−0.09) R_⊕, and ρ_P = 3.32^(+0.86)_(−0.98) g cm^(−3), giving Kepler-68b a density intermediate between that of the ice giants and Earth. Kepler-68c is Earth-sized, with a radius R_P = 0.953^(+0.037)_(−0.042) R_⊕ and transits on a 9.6 day orbit; validation of Kepler-68c posed unique challenges. Kepler-68d has an orbital period of 580 ± 15 days and a minimum mass of M_P sin_i = 0.947 ± 0.035M_J . Power spectra of the Kepler photometry at one minute cadence exhibit a rich and strong set of asteroseismic pulsation modes enabling detailed analysis of the stellar interior. Spectroscopy of the star coupled with asteroseismic modeling of the multiple pulsation modes yield precise measurements of stellar properties, notably T_(eff) = 5793±74 K,M_★ = 1.079±0.051M_☉, R_★ = 1.243±0.019 R_☉, and ρ_★ = 0.7903±0.0054 g cm^(−3), all measured with fractional uncertainties of only a few percent. Models of Kepler-68b suggest that it is likely composed of rock and water, or has a H and He envelope to yield its density ∼3 g cm^(−3).
Nature | 2013
Soren Meibom; Guillermo Torres; Francois Fressin; David W. Latham; Jason F. Rowe; David R. Ciardi; S. T. Bryson; Leslie A. Rogers; Christopher E. Henze; Kenneth A. Janes; Sydney A. Barnes; Geoffrey W. Marcy; Howard Isaacson; Debra A. Fischer; Steve B. Howell; Elliott P. Horch; Jon M. Jenkins; Simon C. Schuler; Justin R. Crepp
Most stars and their planets form in open clusters. Over 95 per cent of such clusters have stellar densities too low (less than a hundred stars per cubic parsec) to withstand internal and external dynamical stresses and fall apart within a few hundred million years. Older open clusters have survived by virtue of being richer and denser in stars (1,000 to 10,000 per cubic parsec) when they formed. Such clusters represent a stellar environment very different from the birthplace of the Sun and other planet-hosting field stars. So far more than 800 planets have been found around Sun-like stars in the field. The field planets are usually the size of Neptune or smaller. In contrast, only four planets have been found orbiting stars in open clusters, all with masses similar to or greater than that of Jupiter. Here we report observations of the transits of two Sun-like stars by planets smaller than Neptune in the billion-year-old open cluster NGC6811. This demonstrates that small planets can form and survive in a dense cluster environment, and implies that the frequency and properties of planets in open clusters are consistent with those of planets around field stars in the Galaxy.
The Astrophysical Journal | 2013
Saul Rappaport; Roberto Sanchis-Ojeda; Leslie A. Rogers; Alan M. Levine; Joshua N. Winn
The requirement that a planet must orbit outside of its Roche limit gives a lower limit on the planets mean density. The minimum density depends almost entirely on the orbital period and is immune to systematic errors in the stellar properties. We consider the implications of this density constraint for the newly identified class of small planets with periods shorter than half a day. When the planets radius is accurately known, this lower limit to the density can be used to restrict the possible combinations of iron and rock within the planet. Applied to KOI 1843.03, a 0.6 R⊕ planet with the shortest known orbital period of 4.245 hr, the planets mean density must be ≳7 g cm^(–3). By modeling the planetary interior subject to this constraint, we find that the composition of the planet must be mostly iron, with at most a modest fraction of silicates (≾30% by mass).
The Astrophysical Journal | 2016
Howard Chen; Leslie A. Rogers
Sub-Neptune-sized exoplanets represent one of the most common types of planets in the Milky Way, yet many of their properties are unknown. Here, we present a prescription to adapt the capabilities of the stellar evolution toolkit Modules for Experiments in Stellar Astrophysics (MESA) to model sub-Neptune mass planets with H/He envelopes. With the addition of routines treating the planet core luminosity, heavy element enrichment, atmospheric boundary condition, and mass loss due to hydrodynamic winds, the evolutionary pathways of planets with diverse starting conditions are more accurately constrained. Using these dynamical models, we construct mass-composition relationships of planets from 1 to 400
The Astrophysical Journal | 2016
Lauren M. Weiss; Leslie A. Rogers; Howard Isaacson; Eric Agol; Geoffrey W. Marcy; Jason F. Rowe; David M. Kipping; Benjamin J. Fulton; Jack J. Lissauer; Andrew W. Howard; Daniel C. Fabrycky
M_{\oplus}