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Dive into the research topics where Robert D. Reasenberg is active.

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Featured researches published by Robert D. Reasenberg.


Science | 1974

Venus - Mass, gravity field, atmosphere, and ionosphere as measured by the Mariner 10 dual-frequency radio system

H. T. Howard; G. L. Tyler; Gunnar Fjeldbo; A. J. Kliore; G. S. Levy; D. L. Brunn; R. Dickinson; Robert E. Edelson; W. L. Martin; R. B. Postal; B. L. Seidel; T.T. Sesplaukis; D. L. Shirley; C. T. Stelzried; D. N. Sweetnam; A. I. Zygielbaum; P. B. Esposito; J. D. Anderson; Irwin I. Shapiro; Robert D. Reasenberg

Analysis of the Doppler tracking data near encounter yields a value for the ratio of the mass of the sun to that of Venus of 408,523.9 � 1.2, which is in good agreement with prior determinations based on data from Mariner 2 and Mariner 5. Preliminary analysis indicates that the magnitudes of the fractional differences in the principal moments of inertia of Venus are no larger than 10-4, given that the effects of gravity-field harmonics higher than the second are negligible. Additional analysis is needed to determine the influence of the higher order harmonics on this bound. Four distinct temperature inversions exist at altitudes of 56, 58, 61, and 63 kilometers. The X-band signal was much more rapidly attenuated than the S-band signal and disappeared completely at 52-kilometer altitude. The nightside ionosphere consists of two layers having a peak density of 104 electrons per cubic centimeter at altitudes of 140 and 120 kilometers. The dayside ionosphere has a peak density of 3 X 105 electrons per cubic centimeter at an altitude of 145 kilometers. The electron number density observed at higher altitudes was ten times less than that observed by Mariner 5, and no strong evidence for a well-defined plasmapause was found.


Science | 1974

Mercury - Results on mass, radius, ionosphere, and atmosphere from Mariner 10 dual-frequency radio signals

H. T. Howard; G. L. Tyler; P. B. Esposito; John D. Anderson; Robert D. Reasenberg; Irwin I. Shapiro; G. Fjeldbo; Arvydas J. Kliore; G. S. Levy; D. L. Brunn; R. Dickinson; R. E. Edelson; W. L. Martin; R. B. Postal; B. Seidel; T. T. Sesplaukis; D. L. Shirley; C. T. Stelzried; D. N. Sweetnam; G. E. Wood; A. I. Zygielbaum

Analysis of the radio-tracking data from Mariner 10 yields 6,023,600 � 600 for the ratio of the mass of the sun to that of Mercury, in very good agreement with values determined earlier from radar data alone. Occultation measurements yielded values for the radius of Mercury of 2440 � 2 and 2438 � 2 kilometers at laditudes of 2�N and 68�N, respectively, again in close agreement with the average equatorial radius of 2439 � 1 kilometers determined from radar data. The mean density of 5.44 grams per cubic centimeter deduced for Mercury from Mariner 10 data thus virtually coincides with the prior determination. No evidence of either an ionosphere or an atmosphere was found, with the data yielding upper bounds on the electron density of about 1500 and 4000 electrons per cubic centimeter on the dayside and nightside, respectively, and an inferred upper bound on the surface pressure of 10-8 millibar.


Review of Scientific Instruments | 2005

Tracking frequency laser distance gauge

James D. Phillips; Robert D. Reasenberg

Advanced astronomical missions with greatly enhanced resolution and physics missions of unprecedented accuracy will require laser distance gauges of substantially improved performance. We describe a laser gauge, based on Pound–Drever–Hall locking, in which the optical frequency is adjusted to maintain an interferometer’s null condition. This technique has been demonstrated with pm performance. Automatic fringe hopping allows it to track arbitrary distance changes. The instrument is intrinsically free of the nm-scale cyclic bias present in traditional (heterodyne) high-precision laser gauges. The output is a radio frequency, readily measured to sufficient accuracy. The laser gauge has operated in a resonant cavity, which improves precision, can suppress the effects of misalignments, and makes possible precise automatic alignment. The measurement of absolute distance requires little or no additional hardware, and has also been demonstrated. The proof-of-concept version, based on a stabilized HeNe laser and ...


1994 Symposium on Astronomical Telescopes & Instrumentation for the 21st Century | 1994

Current status of the IOTA interferometer

N. P. Carleton; Wesley A. Traub; Marc G. Lacasse; Peter Nisenson; Michael R. Pearlman; Robert D. Reasenberg; Xinqi Xu; Charles M. Coldwell; Alexander Panasyuk; James A. Benson; Costas Papaliolios; Read Predmore; F. Peter Schloerb; H. M. Dyck; David M. Gibson

The first two telescopes of the Infrared-Optical Telescope Array (IOTA) project are now in place and yielding data at the Smithsonian Institutions F. L. Whipple Observatory on Mt. Hopkins, near Tucson, Arizona. The IOTA collectors are 45 cm in diameter, and may be moved to various stations in an L-shaped configuration with a maximum baseline of 38 m. A third collector will be added as soon as funding permits. Each light-collector assembly consists of a siderostat feeding a stationary afocal Cassegrain telescope that produces a 10-X reduced parallel beam, which is in turn directed vertically downward by a piezo-driven active mirror that stabilizes the ultimate image position. The reduced beams enter an evacuated envelope and proceed to the corner of the array, where they are turned back along one arm for path compensation. The delay line, in one beam, consists of two parts: one dihedral reflector positioned in a slew-and-clamp mode to give the major part of the desired delay; and a second dihedral mounted on an air-bearing carriage to provide the variable delay that is needed. After delay, the beams exit from the vacuum and are directed by dichroic mirrors into the infrared beam-combination and detection system. The visible light passes on to another area, to the image-tracker detectors and the visible-light combination and detection system. The beams are combined in pupil-plane mode on beam splitters. The combined IR beams are conveyed to two cooled single-element InSb detectors. The combined visible-light beams are focussed by lenslet arrays onto multimode optical fibers that lead to the slit of a specially-designed prism spectrometer. For the visible mode, the delay line is run at several wavelengths on one side of the zero- path point, so that several cycles of interference occur across the spectrum. First results were obtained with the IR system, giving visibilities for several K and M stars, using 2.2 micrometers radiation on a N-S baseline of 21.2 m. From these measurements we obtained preliminary estimates of effective stellar diameters in the K band.


Proceedings of SPIE | 2008

The Milli-Arc-Second Structure Imager, MASSIM: A New Concept for a High Angular Resolution X-ray Telescope

Gerald K. Skinner; Zaven Arzoumanian; Webster Cash; N. Gehrels; Keith C. Gendreau; Paul Gorenstein; John F. Krizmanic; M. C. Miller; James D. Phillips; Robert D. Reasenberg; Christopher S. Reynolds; Rita M. Sambruna; R. E. Streitmatter; David L. Windt

MASSIM, the Milli-Arc-Second Structure Imager, is a mission that has been proposed for study within the context of NASAs Astrophysics Strategic Mission Concept Studies program. It uses a set of achromatic diffractive-refractive Fresnel lenses on an optics spacecraft to focus 5-11 keV X-rays onto detectors on a second spacecraft flying in formation 1000 km away. It will have a point-source sensitivity comparable with that of the current generation of major X-ray observatories (Chandra, XMM-Newton) but an angular resolution some three orders of magnitude better. MASSIM is optimized for the study of jets and other phenomena that occur in the immediate vicinity of black holes and neutron stars. It can also be used for studying other astrophysical phenomena on the milli-arc-second scale, such as those involving proto-stars, the surfaces and surroundings of nearby active stars and interacting winds. We describe the MASSIM mission concept, scientific objectives and the trade-offs within the X-ray optics design. The anticipated performance of the mission and possible future developments using the diffractive-refractive optics approach to imaging at X-ray and gamma-ray energies are discussed.


Optics Letters | 2011

Subpicometer length measurement using semiconductor laser tracking frequency gauge.

Rajesh Thapa; James D. Phillips; Emanuele Rocco; Robert D. Reasenberg

We have demonstrated heretofore unattained distance precision of 0.14 pm (2 pm) incremental and 14 nm (2.9 μm) absolute in a resonant (nonresonant) interferometer at an averaging time of 1 s, using inexpensive telecommunications diode lasers. We have controlled the main source of error, that due to spurious reflection and the resulting amplitude modulation. In the resonant interferometer, absolute distance precision is well under λ/6. Therefore, after an interruption, an absolute distance measurement can be used to return to the same interferometer order.


The Astronomical Journal | 1995

First 2.2 micrometer results from the IOTA interferometer

Hm Dyck; Ja Benson; N. P. Carlton; C. Coldwell; Marc G. Lacasse; P. Nisenson; A. Panasyuk; C. Papaliolios; R. D. Pearlman; Robert D. Reasenberg

We present the first infrared fringe visibility measurements made with the Infrared Optical Telescope Array on Mt. Hopkins. Effective temperatures are derived for RX Boo, RS Cnc, and Beta Peg. RX Boo is the coolest small-amplitude variable giant star to have an effective temperature determination. We compare the size of its photosphere at infrared wavelengths with the sizes of its SiO and H20 radio emission regions. We also discuss initial performance parameters for the interferometer.


Astronomical Telescopes and Instrumentation | 2000

Full-sky Astrometric Mapping Explorer: an optical astrometric survey mission

Scott D. Horner; Marvin Edward Germain; Frederick H. Harris; Mark S. Johnson; K. J. Johnston; David G. Monet; Marc A. Murison; James D. Phillips; Robert D. Reasenberg; P. Kenneth Seidelmann; S. E. Urban; Richard H. Vassar

The Full-sky Astrometric Mapping Explorer (FAME) is a MIDEX class Explorer mission designed to perform an all-sky, astrometric survey with unprecedented accuracy, determining the positions, parallaxes, proper motions, and photometry of 40 million stars. It will create a rigid, astrometric catalog of stars from an input catalog with 5 < mv < 15. For bright stars, 5 < mv < 9, FAMEs goal is to determine positions and parallaxes accurate to < 50 (mu) as, with proper motion errors < 50 (mu) as/year. For fainter stars, 9 < mv < 15, FAMEs goal is to determine positions and parallaxes accurate to < 500 (mu) as, with proper motion errors < 500 (mu) as/year. It will also collect photometric data on these 40 million stars in four Sloan DSS colors.


Classical and Quantum Gravity | 2011

A quick test of the WEP enabled by a sounding rocket

Robert D. Reasenberg; Enrico C. Lorenzini; Biju R. Patla; James D. Phillips; Eugeniu E. Popescu; Emanuele Rocco; Rajesh Thapa

We describe SR-POEM, a Galilean test of the weak equivalence principle (WEP), which is to be conducted during the free fall portion of a sounding rocket flight. This test of a single pair of substances is aimed at a measurement uncertainty of σ(η) < 10–16 after averaging the results of eight separate drops, each of 40 s duration. The WEP measurement is made with a set of four laser gauges that are expected to achieve 0.1 pm Hz–1/2. We address the two sources of systematic error that are currently of greatest concern: magnetic force and electrostatic (patch effect) force on the test mass assemblies. The discovery of a violation (η ≠ 0) would have profound implications for physics, astrophysics and cosmology.


Classical and Quantum Gravity | 2010

A weak equivalence principle test on a suborbital rocket

Robert D. Reasenberg; James D. Phillips

We describe a Galilean test of the weak equivalence principle, to be conducted during the free fall portion of a sounding rocket flight. The test of a single pair of substances is aimed at a measurement uncertainty of ?(?) < 10?16 after averaging the results of eight separate drops. The weak equivalence principle measurement is made with a set of four laser gauges that are expected to achieve 0.1 pm Hz?1/2. The discovery of a violation (? ? 0) would have profound implications for physics, astrophysics and cosmology.

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James D. Phillips

Smithsonian Astrophysical Observatory

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Robert William Babcock

Smithsonian Astrophysical Observatory

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Irwin I. Shapiro

Massachusetts Institute of Technology

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Marc A. Murison

Smithsonian Astrophysical Observatory

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Martin Charles Noecker

Smithsonian Astrophysical Observatory

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K. J. Johnston

United States Naval Research Laboratory

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