Jason D. Eastman
Harvard University
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Publications of the Astronomical Society of the Pacific | 2010
Jason D. Eastman; Robert Siverd; B. Scott Gaudi
As the quality and quantity of astrophysical data continue to improve, the precision with which certain astrophysical events can be timed becomes limited not by the data themselves, but by the manner, standard, and uniformity with which time itself is referenced. While some areas of astronomy (most notably pulsar studies) have required absolute time stamps with precisions of considerably better than 1 minute for many decades, recently new areas have crossed into this regime. In particular, in the exoplanet community, we have found that the (typically unspecified) time standards adopted by various groups can differ by as much as a minute. Left uncorrected, this ambiguity may be mistaken for transit timing variations and bias eccentricity measurements. We argue that, since the commonly-used Julian Date, as well as its heliocentric and barycentric counterparts, can be specified in several time standards, it is imperative that their time standards always be reported when accuracies of 1 minute are required. We summarize the rationale behind our recommendation to quote the site arrival time, in addition to using BJDTDB, the Barycentric Julian Date in the Barycentric Dynamical Time standard for any astrophysical event. The BJDTDB is the most practical absolute time stamp for extraterrestrial phenomena, and is ultimately limited by the properties of the target system. We compile a general summary of factors that must be considered in order to achieve timing precisions ranging from 15 minutes to 1 μs. Finally, we provide software tools that, in principal, allow one to calculate BJDTDB to a precision of 1 μs for any target from anywhere on Earth or from any spacecraft.
The Astronomical Journal | 2008
Joshua A. Frieman; Bruce A. Bassett; Andrew Cameron Becker; Changsu Choi; D. Cinabro; F. DeJongh; D. L. DePoy; Ben Dilday; Mamoru Doi; Peter Marcus Garnavich; Craig J. Hogan; Jon A. Holtzman; Myungshin Im; Saurabh W. Jha; Richard Kessler; Kohki Konishi; Hubert Lampeitl; John P. Marriner; J. L. Marshall; David P. McGinnis; Gajus A. Miknaitis; Robert C. Nichol; Jose Luis Palacio Prieto; Adam G. Riess; Michael W. Richmond; Roger W. Romani; Masao Sako; Donald P. Schneider; Mathew Smith; Naohiro Takanashi
The Sloan Digital Sky Survey-II (SDSS-II) has embarked on a multi-year project to identify and measure light curves for intermediate-redshift (0.05 < z < 0.35) Type Ia supernovae (SNe Ia) using repeated five-band (ugriz) imaging over an area of 300 sq. deg. The survey region is a stripe 2.5° wide centered on the celestial equator in the Southern Galactic Cap that has been imaged numerous times in earlier years, enabling construction of a deep reference image for the discovery of new objects. Supernova imaging observations are being acquired between September 1 and November 30 of 2005-7. During the first two seasons, each region was imaged on average every five nights. Spectroscopic follow-up observations to determine supernova type and redshift are carried out on a large number of telescopes. In its first two three-month seasons, the survey has discovered and measured light curves for 327 spectroscopically confirmed SNe Ia, 30 probable SNe Ia, 14 confirmed SNe Ib/c, 32 confirmed SNe II, plus a large number of photometrically identified SNe Ia, 94 of which have host-galaxy spectra taken so far. This paper provides an overview of the project and briefly describes the observations completed during the first two seasons of operation.
The Astrophysical Journal | 2010
K. D. Denney; Bradley M. Peterson; Richard W. Pogge; A. Adair; David W. Atlee; K. Au-Yong; Misty C. Bentz; Jonathan C. Bird; D. J. Brokofsky; E. Chisholm; M. L. Comins; Matthias Dietrich; V. T. Doroshenko; Jason D. Eastman; Yu. S. Efimov; S. Ewald; S. Ferbey; C. M. Gaskell; C. H. Hedrick; K. Jackson; S.A. Klimanov; Elizabeth S. Klimek; A. K. Kruse; A. Ladéroute; J. B. Lamb; Karen M. Leighly; Takeo Minezaki; S. V. Nazarov; Christopher A. Onken; Eric A. Petersen
We present the final results from a high sampling rate, multi-month, spectrophotometric reverberation mapping campaign undertaken to obtain either new or improved Hβ reverberation lag measurements for several relatively low-luminosity active galactic nuclei (AGNs). We have reliably measured the time delay between variations in the continuum and Hβ emission line in six local Seyfert 1 galaxies. These measurements are used to calculate the mass of the supermassive black hole at the center of each of these AGNs. We place our results in context to the most current calibration of the broad-line region (BLR) RBLR–L relationship, where our results remove outliers and reduce the scatter at the low-luminosity end of this relationship. We also present velocity-resolved Hβ time-delay measurements for our complete sample, though the clearest velocity-resolved kinematic signatures have already been published.
Publications of the Astronomical Society of the Pacific | 2013
Jason D. Eastman; B. Scott Gaudi; Eric Agol
We present EXOFAST, a fast, robust suite of routines written in IDL that is designed to fit exoplanetary transits and radial velocity variations simultaneously or separately and characterize the parameter uncertainties and covariances with a differential evolution Markov chain Monte Carlo method. We describe how our code incorporates both data sets to derive simultaneously stellar parameters along with the transit and RV parameters, resulting in more self-consistent results on an example fit of the discovery data of HAT-P-3b that is well-mixed in under 5 minutes on a standard desktop computer. We describe in detail how our code works and outline ways in which the code can be extended to include additional effects or generalized for the characterization of other data sets—including non-planetary data sets. We discuss the pros and cons of several common ways to parameterize eccentricity, highlight a subtle mistake in the implementation of MCMC that could bias the inferred eccentricity of intrinsically circular orbits to significantly non-zero results, discuss a problem with IDLs built-in random number generator in its application to large MCMC fits, and derive a method to analytically fit the linear and quadratic limb darkening coefficients of a planetary transit. Finally, we explain how we achieved improved accuracy and over a factor of 100 improvement in the execution time of the transit model calculation. Our entire source code, along with an easy-to-use online interface for several basic features of our transit and radial velocity fitting, are available online at http://astroutils.astronomy.ohio-state.edu/exofast.
Publications of the Astronomical Society of the Pacific | 2007
Mark M. Phillips; Weidong Li; Joshua A. Frieman; Sergei I. Blinnikov; D. L. DePoy; Jose Luis Palacio Prieto; Peter A. Milne; Carlos Contreras; Gaston Folatelli; Nidia I. Morrell; Mario Hamuy; Nicholas B. Suntzeff; M. Roth; Sergio Gonzalez; Wojtek Krzeminski; Alexei V. Filippenko; Wendy L. Freedman; Ryan Chornock; Saurabh W. Jha; Barry F. Madore; S. E. Persson; Christopher R. Burns; P. Wyatt; David C. Murphy; Ryan J. Foley; Mohan Ganeshalingam; F. J. D. Serduke; Kevin Krisciunas; Bruce A. Bassett; Andrew Cameron Becker
ABSTRACT We present extensive \documentclass{aastex} \usepackage{amsbsy} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{bm} \usepackage{mathrsfs} \usepackage{pifont} \usepackage{stmaryrd} \usepackage{textcomp} \usepackage{portland,xspace} \usepackage{amsmath,amsxtra} \usepackage[OT2,OT1]{fontenc} \newcommand\cyr{ \renewcommand\rmdefault{wncyr} \renewcommand\sfdefault{wncyss} \renewcommand\encodingdefault{OT2} \normalfont \selectfont} \DeclareTextFontCommand{\textcyr}{\cyr} \pagestyle{empty} \DeclareMathSizes{10}{9}{7}{6} \begin{document} \landscape
The Astrophysical Journal | 2012
Robert J. Siverd; Thomas G. Beatty; Joshua Pepper; Jason D. Eastman; Karen A. Collins; Allyson Bieryla; David W. Latham; Lars A. Buchhave; Eric L. N. Jensen; Justin R. Crepp; R. A. Street; Keivan G. Stassun; B. Scott Gaudi; Perry L. Berlind; Michael L. Calkins; D. L. DePoy; Gilbert A. Esquerdo; Benjamin J. Fulton; Gábor Fűrész; John C. Geary; Andrew Gould; L. Hebb; John F. Kielkopf; J. L. Marshall; Richard W. Pogge; K. Z. Stanek; Robert P. Stefanik; Andrew Szentgyorgyi; Mark Trueblood; Patricia Trueblood
u^{\prime }g^{\prime }r^{\prime }i^{\prime }BVRIYJHK_{s}
Nature | 2015
Andrew Vanderburg; John Asher Johnson; Saul Rappaport; Allyson Bieryla; J. Irwin; John Arban Lewis; David M. Kipping; Warren R. Brown; P. Dufour; David R. Ciardi; Ruth Angus; Laura Schaefer; David W. Latham; David Charbonneau; Charles A. Beichman; Jason D. Eastman; Nate McCrady; Robert A. Wittenmyer; Jason T. Wright
\end{document} photometry and optical spectroscopy of the Type Ia supernova (SN) 2005hk. These data reveal that SN 2005hk was nearly identical in its observed properties to SN 2002cx, which has been called “the most peculiar known Type Ia supernova.” Both supernovae exhibited high‐ionization SN 1991T–like premaximum spectra, yet low peak luminosities like that of SN 1991bg. The spectra reveal th...
The Astrophysical Journal | 2008
Joshua A. Carter; J. C. Yee; Jason D. Eastman; B. Scott Gaudi; Joshua N. Winn
We present the discovery of KELT-1b, the first transiting low-mass companion from the wide-field Kilodegree Extremely Little Telescope-North (KELT-North) transit survey. A joint analysis of the spectroscopic, radial velocity, and photometric data indicates that the V = 10.7 primary is a mildly evolved mid-F star with Teff = 6516±49 K, log g = 4.228 +0.014 −0.021, and [Fe/H] = 0.052±0.079, with an inferred mass M∗ = 1.335 ± 0.063 M� and radius R∗ = 1.471 +0.045 −0.035 R� . The companion is a low-mass brown dwarf or a super-massive planet with mass MP = 27.38 ± 0.93 MJup and radius RP = 1.116 +0.038 −0.029 RJup. The companion is on a very short (∼29 hr) period circular orbit, with an ephemeris Tc(BJDTDB) = 2455909.29280 ± 0.00023 and P = 1.217501 ± 0.000018 days. KELT-1b receives a large amount of stellar insolation, resulting in an estimated equilibrium temperature assuming zero albedo and perfect redistribution of Teq = 2423 +3427 K. Comparison with standard evolutionary models suggests that the radius of KELT-1b is likely to be significantly inflated. Adaptive optics imaging reveals a candidate stellar companion to KELT-1 with a separation of 588 ± 1 mas, which is consistent with an M dwarf if it is at the same distance as the primary. Rossiter–McLaughlin measurements during transit imply a projected spin–orbit alignment angle λ = 2 ± 16 deg, consistent with a zero obliquity for KELT-1. Finally, the v sin I∗ = 56 ± 2k m s −1 of the primary is consistent at ∼2σ with tidal synchronization. Given the extreme parameters of the KELT-1 system, we expect it to provide an important testbed for theories of the emplacement and evolution of short-period companions, as well as theories of tidal dissipation and irradiated brown dwarf atmospheres.
The Astrophysical Journal | 2009
K. D. Denney; Lorna Watson; Bradley M. Peterson; Richard W. Pogge; David W. Atlee; Misty C. Bentz; Jonathan C. Bird; D. J. Brokofsky; M. L. Comins; Matthias Dietrich; V. T. Doroshenko; Jason D. Eastman; Yu. S. Efimov; C. M. Gaskell; C. H. Hedrick; S. A. Klimanov; Elizabeth S. Klimek; A. K. Kruse; J. B. Lamb; Karen M. Leighly; Takeo Minezaki; S. V. Nazarov; Eric A. Petersen; P. Peterson; Shawn Poindexter; Y. Schlesinger; K. J. Sakata; S. G. Sergeev; John J. Tobin; Cayman T. Unterborn
Most stars become white dwarfs after they have exhausted their nuclear fuel (the Sun will be one such). Between one-quarter and one-half of white dwarfs have elements heavier than helium in their atmospheres, even though these elements ought to sink rapidly into the stellar interiors (unless they are occasionally replenished). The abundance ratios of heavy elements in the atmospheres of white dwarfs are similar to the ratios in rocky bodies in the Solar System. This fact, together with the existence of warm, dusty debris disks surrounding about four per cent of white dwarfs, suggests that rocky debris from the planetary systems of white-dwarf progenitors occasionally pollutes the atmospheres of the stars. The total accreted mass of this debris is sometimes comparable to the mass of large asteroids in the Solar System. However, rocky, disintegrating bodies around a white dwarf have not yet been observed. Here we report observations of a white dwarf—WD 1145+017—being transited by at least one, and probably several, disintegrating planetesimals, with periods ranging from 4.5 hours to 4.9 hours. The strongest transit signals occur every 4.5 hours and exhibit varying depths (blocking up to 40 per cent of the star’s brightness) and asymmetric profiles, indicative of a small object with a cometary tail of dusty effluent material. The star has a dusty debris disk, and the star’s spectrum shows prominent lines from heavy elements such as magnesium, aluminium, silicon, calcium, iron, and nickel. This system provides further evidence that the pollution of white dwarfs by heavy elements might originate from disrupted rocky bodies such as asteroids and minor planets.
The Astrophysical Journal | 2009
K. D. Denney; Bradley M. Peterson; Richard W. Pogge; A. Adair; David W. Atlee; K. Au-Yong; Misty C. Bentz; Jonathan C. Bird; D. J. Brokofsky; E. Chisholm; M. L. Comins; Matthias Dietrich; V. T. Doroshenko; Jason D. Eastman; Yu. S. Efimov; S. Ewald; S. Ferbey; C. M. Gaskell; C. H. Hedrick; K. Jackson; S. A. Klimanov; Elizabeth S. Klimek; A. K. Kruse; A. Ladéroute; J. B. Lamb; Karen M. Leighly; Takeo Minezaki; S. V. Nazarov; Christopher A. Onken; Eric A. Petersen
The light curve of an exoplanetary transit can be used to estimate the planetary radius and other parameters of interest. Because accurate parameter estimation is a nonanalytic and computationally intensive problem, it is often useful to have analytic approximations for the parameters as well as their uncertainties and covariances. Here, we give such formulae, for the case of an exoplanet transiting a star with a uniform brightness distribution. We also assess the advantages of some relatively uncorrelated parameter sets for fitting actual data. When limb darkening is significant, our parameter sets are still useful, although our analytic formulae underpredict the covariances and uncertainties.