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Dive into the research topics where G. Hamilton is active.

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Featured researches published by G. Hamilton.


Nature | 2007

The lakes of Titan

Ellen R. Stofan; Charles Elachi; Jonathan I. Lunine; Ralph D. Lorenz; Bryan W. Stiles; K. L. Mitchell; S. Ostro; L. Soderblom; C. Wood; Howard A. Zebker; Stephen D. Wall; M. Janssen; Randolph L. Kirk; Rosaly M. C. Lopes; F. Paganelli; Jani Radebaugh; L. Wye; Y. Anderson; M. Allison; R. A. Boehmer; Philip S. Callahan; P. Encrenaz; Enrico Flamini; G. Francescetti; Yonggyu Gim; G. Hamilton; Scott Hensley; William T. K. Johnson; K. D. Kelleher; Duane O. Muhleman

The surface of Saturn’s haze-shrouded moon Titan has long been proposed to have oceans or lakes, on the basis of the stability of liquid methane at the surface. Initial visible and radar imaging failed to find any evidence of an ocean, although abundant evidence was found that flowing liquids have existed on the surface. Here we provide definitive evidence for the presence of lakes on the surface of Titan, obtained during the Cassini Radar flyby of Titan on 22 July 2006 (T16). The radar imaging polewards of 70° north shows more than 75 circular to irregular radar-dark patches, in a region where liquid methane and ethane are expected to be abundant and stable on the surface. The radar-dark patches are interpreted as lakes on the basis of their very low radar reflectivity and morphological similarities to lakes, including associated channels and location in topographic depressions. Some of the lakes do not completely fill the depressions in which they lie, and apparently dry depressions are present. We interpret this to indicate that lakes are present in a number of states, including partly dry and liquid-filled. These northern-hemisphere lakes constitute the strongest evidence yet that a condensable-liquid hydrological cycle is active in Titan’s surface and atmosphere, in which the lakes are filled through rainfall and/or intersection with the subsurface ‘liquid methane’ table.


Nature | 2006

Titan Radar Mapper observations from Cassini's T3 fly-by

Charles Elachi; S. D. Wall; Michael A. Janssen; Ellen R. Stofan; Rosaly M. C. Lopes; R. Kirk; Ralph D. Lorenz; Jonathan I. Lunine; Federica Paganelli; L. Soderblom; C. Wood; Lauren C. Wye; Howard A. Zebker; Y. Z. Anderson; S. Ostro; M. Allison; R. A. Boehmer; Philip S. Callahan; P. Encrenaz; Enrico Flamini; G. Francescetti; Yonggyu Gim; G. Hamilton; Scott Hensley; William L. Johnson; K. D. Kelleher; D. Muhleman; G. Picardi; F. Posa; L. Roth

Cassinis Titan Radar Mapper imaged the surface of Saturns moon Titan on its February 2005 fly-by (denoted T3), collecting high-resolution synthetic-aperture radar and larger-scale radiometry and scatterometry data. These data provide the first definitive identification of impact craters on the surface of Titan, networks of fluvial channels and surficial dark streaks that may be longitudinal dunes. Here we describe this great diversity of landforms. We conclude that much of the surface thus far imaged by radar of the haze-shrouded Titan is very young, with persistent geologic activity.


ieee radar conference | 2008

The UAVSAR instrument: Description and first results

Scott Hensley; Kevin Wheeler; Greg Sadowy; Cathleen E. Jones; Scott Shaffer; Howard A. Zebker; T. Miller; Brandon Heavey; Ernie Chuang; Roger Chao; Ken Vines; Kouji Nishimoto; Jack Prater; Bruce Carrico; Neil Chamberlain; Joanne Shimada; Marc Simard; Bruce Chapman; Ron Muellerschoen; Charles Le; Thierry Michel; G. Hamilton; David Robison; Greg Neumann; Robert Meyer; Phil Smith; Jim Granger; Paul A. Rosen; Dennis A. Flower; Robert A. Smith

The UAVSAR instrument, employing an L-band actively electronically scanned antenna, had its genesis in the ESTO Instrument Incubator Program and after 3 years of development has begun collecting engineering and science data. System design was motivated by solid Earth applications where repeat pass radar interferometry can be used to measure subtle deformation of the surface, however flexibility and extensibility to support other applications were also major design drivers. In fact a Ka-band single-pass radar interferometer for making high precision topographic maps of ice sheets is being developed based to a large extent on components of the UAVSAR L-band radar. By designing the radar to be housed in an external unpressurized pod, it has the potential to be readily ported to many platforms. Initial testing is being carried out with the NASA Gulfstream III aircraft, which has been modified to accommodate the radar pod and has been equipped with precision autopilot capability developed by NASA Dryden Flight Research Center. With this the aircraft can fly within a 10 m diameter tube on any specified trajectory necessary for repeat-pass radar interferometric applications. To maintain the required pointing for repeat-pass interferometric applications we have employed an actively scanned antenna steered using INU measurement data. This paper presents a brief overview of the radar instrument and some of the first imagery obtained from the system.


IEEE Transactions on Geoscience and Remote Sensing | 2009

Cassini RADAR Sequence Planning and Instrument Performance

Richard D. West; Y. Z. Anderson; R. A. Boehmer; L. Borgarelli; Philip S. Callahan; Charles Elachi; Yonggyu Gim; G. Hamilton; Scott Hensley; Michael A. Janssen; William T. K. Johnson; K. D. Kelleher; Ralph D. Lorenz; S. J. Ostro; L. E. Roth; Scott Shaffer; Bryan W. Stiles; S. D. Wall; Lauren C. Wye; Howard A. Zebker

The Cassini RADAR is a multimode instrument used to map the surface of Titan, the atmosphere of Saturn, the Saturn ring system, and to explore the properties of the icy satellites. Four different active mode bandwidths and a passive radiometer mode provide a wide range of flexibility in taking measurements. The scatterometer mode is used for real aperture imaging of Titan, high-altitude (around 20 000 km) synthetic aperture imaging of Titan and Iapetus, and long range (up to 700 000 km) detection of disk integrated albedos for satellites in the Saturn system. Two SAR modes are used for high- and medium-resolution (300-1000 m) imaging of Titans surface during close flybys. A high-bandwidth altimeter mode is used for topographic profiling in selected areas with a range resolution of about 35 m. The passive radiometer mode is used to map emission from Titan, from Saturns atmosphere, from the rings, and from the icy satellites. Repeated scans with differing polarizations using both active and passive data provide data that can usefully constrain models of surface composition and structure. The radar and radiometer receivers show very good stability, and calibration observations have provided an absolute calibration good to about 1.3 dB. Relative uncertainties within a pass and between passes can be even smaller. Data are currently being processed and delivered to the planetary data system at quarterly intervals one year after being acquired.


Journal of Geophysical Research | 2001

Cassini Radio Detection and Ranging (RADAR): Earth and Venus observations

Ralph D. Lorenz; Charles Elachi; Richard D. West; William T. K. Johnson; Michael A. Janssen; Mahta Moghaddam; G. Hamilton; O. Liepack; A. Bunker; Luz Roth; S. D. Wall; L. Dente; Domenico Casarano; Francesco Posa

The Cassini Radio Detection and Ranging (RADAR) was operated in scatterometric and radiometric modes during the Venus 1 and Earth swingbys to verify its functionality. At Venus, only the thermal emission from the thick absorbing atmosphere was detected. At Earth both the radar echo and the microwave emission from the surface were detected and reveal ocean surface disturbances, the rough, high, and cold Andes mountains, and surface features including a small reservoir in Brazil. Instrument performance appears to be excellent.


ieee radar conference | 2013

Methods for testing the Mars Science Laboratory's landing radar

Elaine Chapin; Maurio Grando; G. Hamilton; Kyung S. Pak; Brian D. Pollard; Scott J. Shaffer; Chialin Wu

The Mars Science Laboratorys rover named Curiosity successfully landed on Mars on August 6, 2012. One component of the Mars Science Laboratory (MSL) Entry, Descent, and Landing (EDL) system was the Terminal Descent Sensor (TDS) landing radar. In this paper we describe laboratory testing of this radar performed before launch.


ieee international symposium on phased array systems and technology | 2010

UAVSAR Active Electronically-Scanned Array

Gregory A. Sadowy; Kyle Brown; Neil Chamberlain; Harry Figueroa; Charlie Fisher; Maurio Grando; G. Hamilton; Vatche Vorperian; Mark Zawadzki

The Uninhabited Airborne Vehicle Synthetic Aperture Radar (UAVSAR) is an L-band (1.2–1.3 GHz) repeat pass, interferometric synthetic aperture radar (InSAR) used for Earth science applications. Using complex radar images collected during separate passes on time scales of hours to years, changes in surface topography can be measured. Due to variations in aircraft attitude between passes, antenna beam steering is required to replicate the radar look angle from pass-to-pass. This paper describes an Active Electronically Scanned Array (AESA) that provides beam steering capability in the antenna azimuth plane. The array contains 24 transmit/receive modules generating approximately 2800 W of radiated power and is capable of pulse-to-pulse beam steering and polarization agility. Designed for high reliability as well as serviceability, all array electronics are contained in single 178cm×62cm×12cm air-cooled panel suitable for operation up 60,000 ft altitude.


Science | 2006

The Sand Seas of Titan: Cassini RADAR Observations of Longitudinal Dunes

Ralph D. Lorenz; S. D. Wall; Jani Radebaugh; G. M. Boubin; E. Reffet; Michael A. Janssen; Ellen R. Stofan; Rosaly M. C. Lopes; R. Kirk; Charles Elachi; Jonathan I. Lunine; K. L. Mitchell; F. Paganelli; L. A. Soderblom; Charles A. Wood; Lauren C. Wye; Howard A. Zebker; Y. Z. Anderson; S. J. Ostro; Michael E. D. Allison; R. A. Boehmer; Philip S. Callahan; P. Encrenaz; Gian Gabriele Ori; G. Francescetti; Yonggyu Gim; G. Hamilton; Scott Hensley; William L. Johnson; K. D. Kelleher


Science | 2005

Cassini radar views the surface of Titan.

Charles Elachi; Stephen D. Wall; Michael E. D. Allison; Y. Z. Anderson; R. A. Boehmer; Philip S. Callahan; P. Encrenaz; Enrico Flamini; Giorgio Franceschetti; Yonggyu Gim; G. Hamilton; Scott Hensley; Michael A. Janssen; William L. Johnson; K. D. Kelleher; Randolph L. Kirk; Rosaly M. C. Lopes; Ralph D. Lorenz; Jonathan I. Lunine; Duane O. Muhleman; S. J. Ostro; F. Paganelli; Giovanni Picardi; Francesco Posa; Luz Roth; Roberto Seu; Scott Shaffer; L. A. Soderblom; Bryan W. Stiles; Ellen R. Stofan


Icarus | 2007

Cryovolcanic features on Titan's surface as revealed by the Cassini Titan Radar Mapper

Rosaly M. C. Lopes; K. L. Mitchell; Ellen R. Stofan; Jonathan I. Lunine; Ralph D. Lorenz; F. Paganelli; R. Kirk; Charles A. Wood; S. D. Wall; L.E. Robshaw; Ad Fortes; Catherine Dorothy Neish; Jani Radebaugh; E. G. Reffet; S. J. Ostro; Charles Elachi; Michael E. D. Allison; Y. Z. Anderson; R. A. Boehmer; G. M. Boubin; Philip S. Callahan; P. Encrenaz; Enrico Flamini; G. Francescetti; Yonggyu Gim; G. Hamilton; Scott Hensley; Michael A. Janssen; William T. K. Johnson; K. D. Kelleher

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Yonggyu Gim

California Institute of Technology

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Ralph D. Lorenz

Johns Hopkins University Applied Physics Laboratory

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Michael A. Janssen

California Institute of Technology

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Scott Hensley

California Institute of Technology

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K. D. Kelleher

California Institute of Technology

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Philip S. Callahan

California Institute of Technology

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R. A. Boehmer

California Institute of Technology

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William T. K. Johnson

California Institute of Technology

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Charles Elachi

California Institute of Technology

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Y. Z. Anderson

California Institute of Technology

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