Richard G. Lyon
Goddard Space Flight Center
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Featured researches published by Richard G. Lyon.
Applied Optics | 1997
Richard G. Lyon; John E. Dorband; J. M. Hollis
A set of observed noisy Hubble Space Telescope Faint Object Camera point-spread functions is used to recover the combined Hubble and Faint Object Camera wave-front error. The low-spatial-frequency wave-front error is parameterized in terms of a set of 32 annular Zernike polynomials. The midlevel and higher spatial frequencies are parameterized in terms of set of 891 polar-Fourier polynomials. The parameterized wave-front error is used to generate accurate calculated point-spread functions, both pre- and post-COSTAR (corrective optics space telescope axial replacement), suitable for image restoration at arbitrary wavelengths. We describe the phase-retrieval-based recovery process and the phase parameterization. Resultant calculated precorrection and postcorrection point-spread functions are shown along with an estimate of both pre- and post-COSTAR spherical aberration.
The Astrophysical Journal | 2001
Edwin M. Kellogg; Jeffrey Alan Pedelty; Richard G. Lyon
We report Chandra ACIS-S3 X-ray imaging and spectroscopy of the R Aquarii binary system that show a spatially resolved two-sided jet and an unresolved central source. This is the first published report of such an X-ray jet seen in an evolved ∼2–3 M, stellar system. At keV, the X-ray jet extends to both the northeast E ! 1 (NE) and southwest (SW) relative to the central binary system. At keV, R Aqr is a pointlike source 1 ! E ! 7.1 centered on the star system. While both 3.5 cm radio continuum emission and X-ray emission appear coincident in projection and have maximum intensities at ∼7 .5 NE of the central binary system, the next strongest X-ray component is located ∼30 SW of the central binary system and has no radio continuum counterpart. The X-ray jets are likely shock-heated in the recent past and are not in thermal equilibrium. The strongest SW X-ray jet component may have been shocked recently since there is no relic radio emission as expected from an older shock. At the position of the central binary, we detect X-ray emission below 1.6 keV consistent with blackbody emission at K. There is also a prominent 6.4 keV feature, a possible fluorescence or collisionally 6 T ∼ 2 # 10 excited Fe Ka line from an accretion disk or from the wind of the giant star. For this excitation to occur, there must be an unseen hard source of X-rays or particles in the immediate vicinity of the hot star. Such a source would be hidden from view by the surrounding edge-on accretion disk. Subject headings: binaries: symbiotic — circumstellar matter — radio continuum: stars — stars: individual (R Aquarii) — stars: winds, outflows — white dwarfs — X-rays: general
Proceedings of SPIE | 2007
Lee D. Feinberg; Bruce H. Dean; David L. Aronstein; Charles W. Bowers; William L. Hayden; Richard G. Lyon; Ron Shiri; J. Scott Smith; D. Scott Acton; Larkin Carey; Adam R. Contos; Erin Sabatke; John P. Schwenker; Duncan Shields; Tim Towell; Fang Shi; Luis Meza
NASAs Technology Readiness Level (TRL)-6 is documented for the James Webb Space Telescope (JWST) Wavefront Sensing and Control (WFSC) subsystem. The WFSC subsystem is needed to align the Optical Telescope Element (OTE) after all deployments have occurred, and achieves that requirement through a robust commissioning sequence consisting of unique commissioning algorithms, all of which are part of the WFSC algorithm suite. This paper identifies the technology need, algorithm heritage, describes the finished TRL-6 design platform, and summarizes the TRL-6 test results and compliance. Additionally, the performance requirements needed to satisfy JWST science goals as well as the criterion that relate to the TRL-6 Testbed Telescope (TBT) performance requirements are discussed.
Proceedings of SPIE | 2004
Mark Clampin; Gary J. Melnick; Richard G. Lyon; Holland C. Ford; J. Roger P. Angel; Daniel Y. Gezari; David A. Golimowski; George F. Hartig; Martin Harwit; Matt Holman; Garth D. Illingworth; Scott J. Kenyon; Douglas N. C. Lin; Mark S. Marley; Scot S. Olivier; Larry Petro; Dimitar D. Sasselov; Jean Schneider; Sara Seager; Michael Shao; W. B. Sparks; Volker Tolls; Alycia J. Weinberger; Hsiao Smith; Ruth Chaing Carter; Robert A. Woodruff; Brent Hyatt; Stephen E. Kendrick; David Purmot
The Extrasolar Planetary Imaging Coronagraph (EPIC) will provide the first direct measurements of a broad range of fundamental physical characteristics of giant planets in other solar systems. These characteristics include orbital inclination, mass, brightness, color, the presence (or absence) of CH4 and H2O, and orbital or rotational-driven variability. EPIC utilizes a 1.5 meter telescope coupled to a Visible Nulling Coronagraph to achieve these science goals. EPIC has been proposed as a Discovery Mission.
The Astrophysical Journal | 1997
J. M. Hollis; Richard G. Lyon; John E. Dorband; Walter A. Feibelman
We present evidence for subarcsecond changes in the ultraviolet (~2550 A) morphology of the inner 5 arcseconds of the R Aqr jet over a 2 yr period. These data were taken with the Hubble Space Telescope (HST) Faint Object Camera (FOC) when the primary mirror flow was still affecting observations. Images of the R Aqr stellar jet were successfully restored to the original design resolution by completely characterizing the telescope-camera point spread function (PSF) with the aid of phase-retrieval techniques. Thus, a noise-free PSF was employed in the final restorations which utilized the maximum entropy method (MEM). We also present recent imagery obtained with the HST/FOC system after the COSTAR correction mission that provides confirmation of the validity of our restoration methodology. The restored results clearly show that the jet is flowing along the northeast (NE)-southwest (SW) axis with a prominent helical-like structure evident on the stronger NE side of the jet. Transverse velocities increase with increasing distance from the central source, providing a velocity range of 36-235 km s-1. From an analysis of proper motions of the two major ultraviolet jet components, we detect an ~40.2 yr event separation of this apparent enhanced material ejection occurring probably at periastron which is consistent with the suspected ~44 yr binary period; this same analysis shows that the jet is undergoing nonlinear acceleration which suggests that the propulsive force probably results from magnetohydromagnetic effects. The restoration computations and the algorithms employed demonstrate that mining of flawed HST data can be scientifically worthwhile.
Proceedings of the International Astronomical Union | 2005
Richard G. Lyon; Mark Clampin; Robert A. Woodruff; Gopal Vasudevan; Mike Shao; Martin S. Levine; Gary J. Melnick; Volker Tolls; Peter Petrone; Peter Dogoda; Julia Duval; Jian Ge
Visible Nulling Coronagraphy (VNC) is the proposed method of detecting and characterizing exo-solar Jovian planets (null depth
Proceedings of SPIE | 2013
Peter R. Lawson; Ruslan Belikov; Webster Cash; Mark Clampin; Tiffany Glassman; Olivier Guyon; N. J. Kasdin; Brian Kern; Richard G. Lyon; Dimitri Mawet; Dwight Moody; Rocco Samuele; Eugene Serabyn; Dan Sirbu; John T. Trauger
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The Astrophysical Journal | 1997
Richard G. Lyon; J. M. Hollis; John E. Dorband
) for the proposed NASAs Extrasolar Planetary Imaging Coronagraph (EPIC) Clampin & Lyon 2004 and is an approach under evaluation for NASAs Terrestrial Planet Finder (TPF) mission. The VNC approach uses a single unobscured filled-aperture telescope and splits, via a 50:50 beamsplitter, its re-imaged pupil into two paths within a Mach-Zender interferometer. An achromatic PI phase shift is imposed onto one beam path and the two paths are laterally sheared with respect to each other. The two beams are recombined at a second 50:50 beamsplitter. The net effect is that the on axis (stellar) light is transmitted out of the bright interferometer arm while the off-axis (planetary) light is transmitted out of the nulled interferometer arm. The bright output is used for fine pointing control and coarse wavefront control. The nulled output is relayed to the science camera for science imagery and fine wavefront control. The actual transmission pattern, projected on the sky, follows a
Proceedings of SPIE | 2012
Richard G. Lyon; Mark Clampin; Peter Petrone; Udayan Mallik; Timothy J. Madison; Matthew R. Bolcar
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Astronomical Telescopes and Instrumentation | 2003
Alfred B. Schultz; Ian J. E. Jordan; M. C. Kochte; Dorothy A. Fraquelli; Fred C. Bruhweiler; J. M. Hollis; Kenneth G. Carpenter; Richard G. Lyon; Mike A. DiSanti; C. L. Miskey; Jesse Leitner; Richard D. Burns; Scott R. Starin; M. Rodrigue; M.S. Fadali; Dennis L. Skelton; H. M. Hart; F. C. Hamilton; Kwang-Ping Cheng
pattern for a single shear,