Nate B. Lust
University of Central Florida
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Featured researches published by Nate B. Lust.
Nature | 2011
Nikku Madhusudhan; Joseph E. Harrington; Kevin B. Stevenson; Sarah Nymeyer; Christopher J. Campo; P. J. Wheatley; Drake Deming; Jasmina Blecic; Ryan A. Hardy; Nate B. Lust; D. R. Anderson; Andrew Collier-Cameron; Christopher B. T. Britt; William C. Bowman; L. Hebb; C. Hellier; P. F. L. Maxted; Don Pollacco; Richard G. West
The carbon-to-oxygen ratio (C/O) in a planet provides critical information about its primordial origins and subsequent evolution. A primordial C/O greater than 0.8 causes a carbide-dominated interior, as opposed to the silicate-dominated composition found on Earth; the atmosphere can also differ from those in the Solar System. The solar C/O is 0.54 (ref. 3). Here we report an analysis of dayside multi-wavelength photometry of the transiting hot-Jupiter WASP-12b (ref. 6) that reveals C/O ≥ 1 in its atmosphere. The atmosphere is abundant in CO. It is depleted in water vapour and enhanced in methane, each by more than two orders of magnitude compared to a solar-abundance chemical-equilibrium model at the expected temperatures. We also find that the extremely irradiated atmosphere (T > 2,500 K) of WASP-12b lacks a prominent thermal inversion (or stratosphere) and has very efficient day–night energy circulation. The absence of a strong thermal inversion is in stark contrast to theoretical predictions for the most highly irradiated hot-Jupiter atmospheres.
Nature | 2010
Kevin B. Stevenson; Joseph E. Harrington; Sarah Nymeyer; Nikku Madhusudhan; Sara Seager; William C. Bowman; Ryan A. Hardy; Drake Deming; Nate B. Lust
The nearby extrasolar planet GJ 436b—which has been labelled as a ‘hot Neptune’—reveals itself by the dimming of light as it crosses in front of and behind its parent star as seen from Earth. Respectively known as the primary transit and secondary eclipse, the former constrains the planet’s radius and mass, and the latter constrains the planet’s temperature and, with measurements at multiple wavelengths, its atmospheric composition. Previous work using transmission spectroscopy failed to detect the 1.4-μm water vapour band, leaving the planet’s atmospheric composition poorly constrained. Here we report the detection of planetary thermal emission from the dayside of GJ 436b at multiple infrared wavelengths during the secondary eclipse. The best-fit compositional models contain a high CO abundance and a substantial methane (CH4) deficiency relative to thermochemical equilibrium models for the predicted hydrogen-dominated atmosphere. Moreover, we report the presence of some H2O and traces of CO2. Because CH4 is expected to be the dominant carbon-bearing species, disequilibrium processes such as vertical mixing and polymerization of methane into substances such as ethylene may be required to explain the hot Neptune’s small CH4-to-CO ratio, which is at least 105 times smaller than predicted.
The Astrophysical Journal | 2011
Christopher J. Campo; Joseph E. Harrington; Ryan A. Hardy; Kevin B. Stevenson; Sarah Nymeyer; Darin Ragozzine; Nate B. Lust; D. R. Anderson; Andrew Collier-Cameron; Jasmina Blecic; Christopher B. T. Britt; William C. Bowman; P. J. Wheatley; Thomas J. Loredo; Drake Deming; L. Hebb; C. Hellier; P. F. L. Maxted; Don Pollaco; Richard G. West
We observed two secondary eclipses of the exoplanet WASP-12b using the Infrared Array Camera on the Spitzer Space Telescope. The close proximity of WASP-12b to its G-type star results in extreme tidal forces capable of inducing apsidal precession with a period as short as a few decades. This precession would be measurable if the orbit had a significant eccentricity, leading to an estimate of the tidal Love number and an assessment of the degree of central concentration in the planetary interior. An initial ground-based secondary-eclipse phase reported by Lopez-Morales et al. (0.510 ± 0.002) implied eccentricity at the 4.5σ level. The spectroscopic orbit of Hebb et al. has eccentricity 0.049 ± 0.015, a 3σ result, implying an eclipse phase of 0.509 ± 0.007. However, there is a well-documented tendency of spectroscopic data to overestimate small eccentricities. Our eclipse phases are 0.5010 ± 0.0006 (3.6 and 5.8 μm) and 0.5006 ± 0.0007 (4.5 and 8.0 μm). An unlikely orbital precession scenario invoking an alignment of the orbit during the Spitzer observations could have explained this apparent discrepancy, but the final eclipse phase of Lopez-Morales et al. (0.510 ±+0.007 –0.006) is consistent with a circular orbit at better than 2σ. An orbit fit to all the available transit, eclipse, and radial-velocity data indicates precession at <1σ; a non-precessing solution fits better. We also comment on analysis and reporting for Spitzer exoplanet data in light of recent re-analyses.
Publications of the Astronomical Society of Japan | 2018
James Bosch; Robert Armstrong; Steven J. Bickerton; Hisanori Furusawa; Hiroyuki Ikeda; Michitaro Koike; Robert H. Lupton; Sogo Mineo; Paul A. Price; Tadafumi Takata; M. Tanaka; Naoki Yasuda; Yusra AlSayyad; Andrew Cameron Becker; William R. Coulton; Jean Coupon; Jose A. Garmilla; Song Huang; K. Simon Krughoff; Dustin Lang; Alexie Leauthaud; Kian-Tat Lim; Nate B. Lust; Lauren A. MacArthur; Rachel Mandelbaum; Hironao Miyatake; Satoshi Miyazaki; Ryoma Murata; Surhud More; Yuki Okura
In this paper, we describe the optical imaging data processing pipeline developed for the Subaru Telescopes Hyper Suprime-Cam (HSC) instrument. The HSC Pipeline builds on the prototype pipeline being developed by the Large Synoptic Survey Telescopes Data Management system, adding customizations for HSC, large-scale processing capabilities, and novel algorithms that have since been reincorporated into the LSST codebase. While designed primarily to reduce HSC Subaru Strategic Program (SSP) data, it is also the recommended pipeline for reducing general-observer HSC data. The HSC pipeline includes high level processing steps that generate coadded images and science-ready catalogs as well as low-level detrending and image characterizations.
The Astronomical Journal | 2016
Patricio Cubillos; Joseph E. Harrington; Thomas J. Loredo; Nate B. Lust; Jasmina Blecic; Madison Stemm
Time-correlated noise is a significant source of uncertainty when modeling exoplanet light-curve data. A correct assessment of correlated noise is fundamental to determine the true statistical significance of our findings. Here we review three of the most widely used correlated-noise estimators in the exoplanet field, the time-averaging, residual-permutation, and wavelet-likelihood methods. We argue that the residual-permutation method is unsound in estimating the uncertainty of parameter estimates. We thus recommend to refrain from this method altogether. We characterize the behavior of the time averagings rms-vs.-bin-size curves at bin sizes similar to the total observation duration, which may lead to underestimated uncertainties. For the wavelet-likelihood method, we note errors in the published equations and provide a list of corrections. We further assess the performance of these techniques by injecting and retrieving eclipse signals into synthetic and real Spitzer light curves, analyzing the results in terms of the relative-accuracy and coverage-fraction statistics. Both the time-averaging and wavelet-likelihood methods significantly improve the estimate of the eclipse depth over a white-noise analysis (a Markov-chain Monte Carlo exploration assuming uncorrelated noise). However, the corrections are not perfect, when retrieving the eclipse depth from Spitzer datasets, these methods covered the true (injected) depth within the 68\% credible region in only
The Astrophysical Journal | 2012
Kevin B. Stevenson; Joseph E. Harrington; Nate B. Lust; Nikole K. Lewis; Guillaume Montagnier; Julianne I. Moses; Channon Visscher; Jasmina Blecic; Ryan A. Hardy; Patricio Cubillos; Christopher J. Campo
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The Astrophysical Journal | 2014
Patricio Cubillos; Joseph E. Harrington; Nikku Madhusudhan; Andrew S. D. Foster; Nate B. Lust; Ryan A. Hardy; M. Oliver Bowman
45--65\% of the trials. Lastly, we present our open-source model-fitting tool, Multi-Core Markov-Chain Monte Carlo ({MC
Publications of the Astronomical Society of the Pacific | 2014
Nate B. Lust; Daniel Britt; Joseph E. Harrington; Sarah Nymeyer; Kevin B. Stevenson; Emily L. Ross; William C. Bowman; Jonathan Fraine
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The Astrophysical Journal | 2018
Erin Kado-Fong; Jenny E. Greene; David Hendel; Adrian M. Price-Whelan; Johnny P. Greco; Andy D. Goulding; Song Huang; Kathryn V. Johnston; Yutaka Komiyama; Chien-Hsiu Lee; Nate B. Lust; Michael A. Strauss; M. Tanaka
}). This package uses Bayesian statistics to estimate the best-fitting values and the credible regions for the parameters for a (user-provided) model. {MC
Archive | 2011
Nikku Madhusudhan; Joseph E. Harrington; Kevin B. Stevenson; Sarah Nymeyer; Christopher J. Campo; P. J. Wheatley; Drake Deming; Jasmina Blecic; Ryan A. Hardy; Nate B. Lust; David A. Anderson; Andrew Collier-Cameron; Leslie Hebb; C. Hellier; P. F. L. Maxted
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