Paul J. Stomski
W.M. Keck Observatory
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Publications of the Astronomical Society of the Pacific | 2006
Peter L. Wizinowich; David Le Mignant; Antonin H. Bouchez; Randy Campbell; Jason C. Y. Chin; Adam R. Contos; Marcos A. van Dam; Scott K. Hartman; Erik M. Johansson; Robert E. Lafon; Hilton Lewis; Paul J. Stomski; Douglas M. Summers; Curtis G. Brown; Pamela M. Danforth; Claire E. Max; Deanna M. Pennington
The Keck Observatory began science observations with a laser guide star adaptive optics system, the first such system on an 8-10 m class telescope, in late 2004. This new capability greatly extends the scientific potential of the Keck II Telescope, allowing near-diffraction-limited observations in the near-infrared using natural guide stars as faint as 19th magnitude. This paper describes the conceptual approach and technical implementation followed for this system, including lessons learned, and provides an overview of the early science capabilities.
Publications of the Astronomical Society of the Pacific | 2000
Peter L. Wizinowich; D. S. Acton; Christian R. Shelton; Paul J. Stomski; J. Gathright; K. Ho; William Lupton; Kevin Tsubota; Olivier Lai; Claire E. Max; James M. Brase; Jong R. An; Kenneth Avicola; Scot S. Olivier; Donald T. Gavel; Bruce A. Macintosh; Andrea M. Ghez; J. Larkin
ABSTRACT Adaptive optics (AO) is a technology that corrects in real time for the blurring effects of atmospheric turbulence, in principle allowing Earth‐bound telescopes to achieve their diffraction limit and to “see” as clearly as if they were in space. The power of AO using natural guide stars has been amply demonstrated in recent years on telescopes up to 3–4 m in diameter. The next breakthrough in astronomical resolution was expected to occur with the implementation of AO on the new generation of large, 8–10 m diameter telescopes. In this paper we report the initial results from the first of these AO systems, now coming on line on the 10 m diameter Keck II Telescope. The results include the highest angular resolution images ever obtained from a single telescope (0 \documentclass{aastex} \usepackage{amsbsy} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{bm} \usepackage{mathrsfs} \usepackage{pifont} \usepackage{stmaryrd} \usepackage{textcomp} \usepackage{portland,xspace} \usepackage{amsmath,amsx...
Publications of the Astronomical Society of the Pacific | 2006
Marcos A. van Dam; Antonin H. Bouchez; David Le Mignant; Erik M. Johansson; Peter L. Wizinowich; Randy Campbell; Jason C. Y. Chin; Scott K. Hartman; Robert E. Lafon; Paul J. Stomski; Douglas M. Summers
The Keck II Telescope is the first 8-10 m class telescope equipped with a laser guide star adaptive optics (LGS AO) system. Under normal seeing conditions, the LGS AO system produces K-band Strehl ratios between 30% and 40% using bright tip-tilt guide stars, and it works well with tip-tilt guide stars as faint as , with partial correction for stars up to a magnitude fainter. This paper presents the algorithms implemented m p 18 R in the LGS AO system, as well as experimental performance results. A detailed error budget shows excellent agreement between the measured and expected image quality for both bright and faint guide stars.
The Astrophysical Journal | 2005
Andrea M. Ghez; Seth David Hornstein; Jessica R. Lu; Antonin H. Bouchez; D. Le Mignant; M. A. van Dam; Peter L. Wizinowich; K. Matthews; Mark R. Morris; E. E. Becklin; Randy Campbell; Jason C. Y. Chin; Scott K. Hartman; Erik M. Johansson; Robert E. Lafon; Paul J. Stomski; Douglas M. Summers
We present the first Laser Guide Star Adaptive Optics (LGS-AO ) observations of the Galactic center. LGSAO has dramatically improved the quality and robustness with which high angular resolution infrared images of the Galactic center can be obtained with the W. M. Keck II 10-meter telescope. Specifically, Strehl ratios of 0.7 and 0.3 at L’[3.8 µm] and K’[2.1 µm], respectively, are achieved in these LGS-AO images; these are at least a factor of two higher and a factor of four to five more stable ag ainst atmospheric fluctuations than the Strehl ratios delivered thus far with the Keck Natural Guide Star AO system on the Galactic center. Furthermore, these observations are the first that cover a large area (76 ′′ × 76 ′′ ) surrounding the central black hole at diffractionlimited resolution for an 8-10 meter class telescope. Durin g our observations, the infrared counterpart to the central supermassive black hole, Sgr A*-IR, showed signific ant infrared intensity variations, with observed L’ magnitudes ranging from 12.6 to 14.5 mag and a decrease in fl ux density of a factor of two over an 8 minute interval. The faintest end of our L’ detections, 1.3 m Jy (dereddened), is the lowest level of emission yet observed for this source by a factor of 3. No significant varia tion in the location of SgrA*-IR is detected as a function of either wavelength or intensity. Previous claim s of such positional variations are easily attributable to a nearby (0. 09 or 720 AU, projected), extended, very red source, which we suggest arises from a locally heated dust feature. Near a peak in its intensity, we obtaine d the first measurement of SgrA*-IR’s K’-L’ color; its K’-L’ of 3.0 ± 0.2 mag (observed) or 1.4 ± 0.2 (dereddened) corresponds to an intrinsic spectral index of � -0.5 ± 0.3 for F� � � � . This is significantly bluer than other recent infrared meas urements from the literature, which suggest � = -4 ± 1. Because our measurement was taken at a time when Sgr A* was�6 times brighter in the infrared than the other measurements, we posit that the spectral index of the emission arising from the vicinity of our Galaxy’s central black hole may depend on the strength of the flare, with stronger flares giving rise to a higher fraction of high energy electrons in the emit ting region. Subject headings:black hole physics ‐ Galaxy:center — infrared:stars ‐ techniques:high angular resolution
Nature | 2006
Franck Marchis; Daniel Hestroffer; Pascal Descamps; Jerome Berthier; Antonin H. Bouchez; Randall D. Campbell; Jason C. Y. Chin; Marcos A. van Dam; Scott K. Hartman; Erik M. Johansson; Robert E. Lafon; David Le Mignant; Imke de Pater; Paul J. Stomski; Doug Summers; Frederic Vachier; Peter L. Wizinovich; Michael H. Wong
The Trojan population consists of two swarms of asteroids following the same orbit as Jupiter and located at the L4 and L5 stable Lagrange points of the Jupiter–Sun system (leading and following Jupiter by 60°). The asteroid 617 Patroclus is the only known binary Trojan. The orbit of this double system was hitherto unknown. Here we report that the components, separated by 680 km, move around the systems centre of mass, describing a roughly circular orbit. Using this orbital information, combined with thermal measurements to estimate the size of the components, we derive a very low density of 0.8 - 0.1 + 0.2 g cm-3. The components of 617 Patroclus are therefore very porous or composed mostly of water ice, suggesting that they could have been formed in the outer part of the Solar System.
Astronomical Telescopes and Instrumentation | 2000
Peter L. Wizinowich; D. Scott Acton; Olivier Lai; J. Gathright; William Lupton; Paul J. Stomski
First light for the Keck II Natural Guide Star (NGS) Adaptive Optics (AO) facility was on the night of February 4, 1999. On the firs attempt at closing the AO loops the image full-width- at-half-maximum (FWHM) went from 0.6 to 0.04 arcsec at H-band (1.65 micrometer wavelength), with a Strehl ratio of 25%. The AO system became an officially scheduled Keck science facility in August 1999; 30 science nights are scheduled in the first half of 2000. The primary purpose of this paper is to present results from this first year at the telescope.
The Astrophysical Journal | 2001
L. Prato; Andrea M. Ghez; Robert K. Pina; Charles M. Telesco; Robert Scott Fisher; Peter L. Wizinowich; Olivier Lai; D. S. Acton; Paul J. Stomski
This paper presents diffraction-limited 1-18 μm images of the young quadruple star system HD 98800 obtained with the W. M. Keck 10 m telescopes using speckle and adaptive optics imaging at near-infrared wavelengths and direct imaging at mid-infrared wavelengths. The two components of the visual binary, A and B, both themselves spectroscopic binaries, were separable at all wavelengths, allowing us to determine their stellar and circumstellar properties. Combining these observations with spectroscopic data from the literature, we derive an age of ~107 yr, masses of 0.93 and 0.64 M☉, and an inclination angle of 58° for the spectroscopic components of HD 98800 B and an age of ~107 yr and a mass of 1.1 M☉ for HD 98800 Aa. Our data confirm that the large mid-infrared excess is entirely associated with HD 98800 B. This excess exhibits a blackbody temperature of 150 K and a strong 10 μm silicate emission feature. The theoretical equilibrium radius of large, perfectly absorbing, 150 K grains around HD 98800 B is 2.4 AU, suggesting a circumspectroscopic binary distribution. Our observations set important upper limits on the size of the inner dust radius of ~2 AU (from the mid-infrared data) and on the quantity of scattered light of less than 10% (from the H-band data). For an inner radius of 2 AU, the dust distribution must have a height of at least 1 AU to account for the fractional dust luminosity of ~20% LB. Based on the scattered-light limit, the dust grains responsible for the excess emission must have an albedo of less than 0.33. The presence of the prominent silicate emission feature at 10 μm implies dust grain radii of 2 μm. The total mass of the dust is greater than 0.002 M⊕. We conclude that the dust is located in a circumbinary disk around the HD 98800 B spectroscopic binary with an inner gap of ~2 AU and a height of 1 AU, and we speculate that the A-Bc orbital dynamics are responsible for the characteristics of the observed dust in the system.
The Astrophysical Journal | 2005
Michael E. Brown; Antonin H. Bouchez; D. Rabinowitz; Re'em Sari; Chadwick Aaron Trujillo; M. van Dam; Randy Campbell; Jason C. Y. Chin; Scott K. Hartman; Erik M. Johansson; Robert E. Lafon; D. Le Mignant; Paul J. Stomski; Douglas M. Summers; Peter L. Wizinowich
The newly commissioned laser guide star adaptive optics system at Keck Observatory has been used to discover and characterize the orbit of a satellite to the bright Kuiper Belt object 2003 EL_(61). Observations over a 6 month period show that the satellite has a semimajor axis of 49,500 ± 400 km, an orbital period of 49.12 ± 0.03 days, and an eccentricity of 0.050 ± 0.003. The inferred mass of the system is (4.2 ± 0.1) × 10^(21) kg, or ~32% of the mass of Pluto and 28.6% ± 0.7% of the mass of the Pluto-Charon system. Mutual occultations occurred in 1999 and will not occur again until 2138. The orbit is fully consistent neither with one tidally evolved from an earlier closer configuration nor with one evolved inward by dynamical friction from an earlier more distant configuration.
Proceedings of SPIE | 2004
Peter L. Wizinowich; David Le Mignant; Antonin H. Bouchez; Jason C. Y. Chin; Adam R. Contos; Scott K. Hartman; Erik M. Johansson; Robert E. Lafon; Chris Neyman; Paul J. Stomski; Doug Summers; Marcos A. van Dam
The purpose of this paper is to report on new adaptive optics (AO) developments at the W. M. Keck Observatory since the 2002 SPIE meeting. These developments include continued improvements to the natural guide star (NGS) facilities, first light for our laser guide star (LGS) system and the commencement of several new Keck AO initiatives.
The Astrophysical Journal | 2003
M. Mark Colavita; R. L. Akeson; Peter L. Wizinowich; Michael Shao; S. Acton; J. Beletic; J. Bell; J. Berlin; Andrew F. Boden; A. Booth; R. Boutell; Frederic H. Chaffee; D. Chan; J. Chock; R. W. Cohen; S. Crawford; Michelle J. Creech-Eakman; G. Eychaner; C. Felizardo; J. Gathright; G. Hardy; H. Henderson; J. Herstein; M. Hess; E. Hovland; M. Hrynevych; R. L. Johnson; J. Kelley; R. Kendrick; C. Koresko
We present the first science results from the Keck Interferometer, a direct-detection infrared interferometer utilizing the two 10 m Keck telescopes. The instrument and system components are briefly described. We then present observations of the T Tauri object DG Tau, which is resolved by the interferometer. The resolved component has a radius of 0.12-0.24 AU, depending on the assumed stellar and extended component fluxes and the model geometry used. Possible origins and implications of the resolved emission are discussed.