J. A. Haberman
Goddard Space Flight Center
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Featured researches published by J. A. Haberman.
Nature | 2005
Hasso B. Niemann; Sushil K. Atreya; S. J. Bauer; G. R. Carignan; J. E. Demick; R. L. Frost; D. Gautier; J. A. Haberman; D. N. Harpold; D. M. Hunten; G. Israel; Jonathan I. Lunine; W. T. Kasprzak; Tobias Owen; M. Paulkovich; F. Raulin; Eric Raaen; S. H. Way
Saturns largest moon, Titan, remains an enigma, explored only by remote sensing from Earth, and by the Voyager and Cassini spacecraft. The most puzzling aspects include the origin of the molecular nitrogen and methane in its atmosphere, and the mechanism(s) by which methane is maintained in the face of rapid destruction by photolysis. The Huygens probe, launched from the Cassini spacecraft, has made the first direct observations of the satellites surface and lower atmosphere. Here we report direct atmospheric measurements from the Gas Chromatograph Mass Spectrometer (GCMS), including altitude profiles of the constituents, isotopic ratios and trace species (including organic compounds). The primary constituents were confirmed to be nitrogen and methane. Noble gases other than argon were not detected. The argon includes primordial 36Ar, and the radiogenic isotope 40Ar, providing an important constraint on the outgassing history of Titan. Trace organic species, including cyanogen and ethane, were found in surface measurements.
Journal of Geophysical Research | 1998
H. B. Niemann; Sushil K. Atreya; G. R. Carignan; T. M. Donahue; J. A. Haberman; D. N. Harpold; R. E. Hartle; D. M. Hunten; W. T. Kasprzak; Paul R. Mahaffy; Tobias Owen; S. H. Way
The Galileo probe mass spectrometer determined the composition of the Jovian atmosphere for species with masses between 2 and 150 amu from 0.5 to 21.1 bars. This paper presents the results of analysis of some of the constituents detected: H2, He, Ne, Ar, Kr, Xe, CH4, NH3, H2O, H2S, C2 and C3 nonmethane hydrocarbons, and possibly PH3 and Cl. 4He/H2 in the Jovian atmosphere was measured to be 0.157 +/- 0.030. 13C/C12 was found to be 0.0108 +/- 0.0005, and D/H and 3He/4He were measured. Ne was depleted, < or = 0.13 times solar, Ar < or = 1.7 solar, Kr < or = 5 solar, and Xe < or = 5 solar. CH4 has a constant mixing ratio of (2.1 +/- 0.4) x 10(-3) (12C, 2.9 solar), where the mixing ratio is relative to H2. Upper limits to the H2O mixing ratio rose from 8 x 10(-7) at pressures <3.8 bars to (5.6 +/- 2.5) x 10(-5) (16O, 0.033 +/- 0.015 solar) at 11.7 bars and, provisionally, about an order of magnitude larger at 18.7 bars. The mixing ratio of H2S was <10(-6) at pressures less than 3.8 bars but rose from about 0.7 x 10(-5) at 8.7 bars to about 7.7 x 10(-5) (32S, 2.5 solar) above 15 bars. Only very large upper limits to the NH3 mixing ratio have been set at present. If PH3 and Cl were present, their mixing ratios also increased with pressure. Species were detected at mass peaks appropriate for C2 and C3 hydrocarbons. It is not yet clear which of these were atmospheric constituents and which were instrumentally generated. These measurements imply (1) fractionation of 4He, (2) a local, altitude-dependent depletion of condensables, probably because the probe entered the descending arm of a circulation cell, (3) that icy planetesimals made significant contributions to the volatile inventory, and (4) a moderate decrease in D/H but no detectable change in (D + 3He)/H in this part of the galaxy during the past 4.6 Gyr.
Science | 1996
Hasso B. Niemann; Sushil K. Atreya; G. R. Carignan; T. M. Donahue; J. A. Haberman; Dan N. Harpold; R. E. Hartle; Donald M. Hunten; W. T. Kasprzak; Paul R. Mahaffy; Tobias Owen; N. W. Spencer; S. H. Way
The composition of the jovian atmosphere from 0.5 to 21 bars along the descent trajectory was determined by a quadrupole mass spectrometer on the Galileo probe. The mixing ratio of He (helium) to H2 (hydrogen), 0.156, is close to the solar ratio. The abundances of methane, water, argon, neon, and hydrogen sulfide were measured; krypton and xenon were detected. As measured in the jovian atmosphere, the amount of carbon is 2.9 times the solar abundance relative to H2, the amount of sulfur is greater than the solar abundance, and the amount of oxygen is much less than the solar abundance. The neon abundance compared with that of hydrogen is about an order of magnitude less than the solar abundance. Isotopic ratios of carbon and the noble gases are consistent with solar values. The measured ratio of deuterium to hydrogen (D/H) of (5 ± 2) × 10−5 indicates that this ratio is greater in solar-system hydrogen than in local interstellar hydrogen, and the 3He/4He ratio of (1.1 ± 0.2) × 10−4 provides a new value for protosolar (solar nebula) helium isotopes. Together, the D/H and 3He/4He ratios are consistent with conversion in the sun of protosolar deuterium to present-day 3He.
Space Science Reviews | 2002
Hasso B. Niemann; Sushil K. Atreya; S. J. Bauer; K. Biemann; Bruce P. Block; G. R. Carignan; T. M. Donahue; R. L. Frost; Daniel Gautier; J. A. Haberman; D. N. Harpold; D. M. Hunten; G. Israel; Jonathan I. Lunine; Konrad Mauersberger; Tobias Owen; F. Raulin; J. E. Richards; S. H. Way
The Gas Chromatograph Mass Spectrometer (GCMS) on the Huygens Probe will measure the chemical composition of Titans atmosphere from 170 km altitude (∼1 hPa) to the surface (∼1500 hPa) and determine the isotope ratios of the major gaseous constituents. The GCMS will also analyze gas samples from the Aerosol Collector Pyrolyser (ACP) and may be able to investigate the composition (including isotope ratios) of several candidate surface materials.The GCMS is a quadrupole mass filter with a secondary electron multiplier detection system and a gas sampling system providing continuous direct atmospheric composition measurements and batch sampling through three gas chromatographic (GC) columns. The mass spectrometer employs five ion sources sequentially feeding the mass analyzer. Three ion sources serve as detectors for the GC columns and two are dedicated to direct atmosphere sampling and ACP gas sampling respectively. The instrument is also equipped with a chemical scrubber cell for noble gas analysis and a sample enrichment cell for selective measurement of high boiling point carbon containing constituents. The mass range is 2 to 141 Dalton and the nominal detection threshold is at a mixing ratio of 10− 8. The data rate available from the Probe system is 885 bit/s. The weight of the instrument is 17.3 kg and the energy required for warm up and 150 minutes of operation is 110 Watt-hours.
Advances in Space Research | 1998
Hasso B. Niemann; Sushil K. Atreya; G. R. Carignan; T. M. Donahue; J. A. Haberman; D. N. Harpold; R. E. Hartle; D. M. Hunten; W. T. Kasprzak; Paul R. Mahaffy; Tobias Owen; N. W. Spencer
The Galileo Probe entered the atmosphere of Jupiter on December 7, 1995. Measurements of the chemical and isotopic composition of the Jovian atmosphere were obtained by the mass spectrometer during the descent over the 0.5 to 21 bar pressure region over a time period of approximately 1 hour. The sampling was either of atmospheric gases directly introduced into the ion source of the mass spectrometer through capillary leaks or of gas, which had been chemically processed to enhance the sensitivity of the measurement to trace species or noble gases. The analysis of this data set continues to be refined based on supporting laboratory studies on an engineering unit. The mixing ratios of the major constituents of the atmosphere hydrogen and helium have been determined as well as mixing ratios or upper limits for several less abundant species including: methane, water, ammonia, ethane, ethylene, propane, hydrogen sulfide, neon, argon, krypton, and xenon. Analysis also suggests the presence of trace levels of other 3 and 4 carbon hydrocarbons, or carbon and nitrogen containing species, phosphine, hydrogen chloride, and of benzene. The data set also allows upper limits to be set for many species of interest which were not detected. Isotope ratios were measured for 3He/4He, D/H, 13C/12C, 20Ne/22Ne, 38Ar/36Ar and for isotopes of both Kr and Xe.
Journal of Geophysical Research | 2010
Hasso B. Niemann; Sushil K. Atreya; J. E. Demick; Daniel Gautier; J. A. Haberman; D. N. Harpold; W. T. Kasprzak; Jonathan I. Lunine; Tobias Owen; F. Raulin
Planetary and Space Science | 2008
O. Witasse; Lyle Huber; Joe Zender; J.-P. Lebreton; R. F. Beebe; David J. Heather; Dennis L. Matson; John C. Zarnecki; Joe Wheadon; Roland Trautner; Marty Tomasko; Piero Leon Stoppato; Fernando Simões; Chuck See; Miguel Pérez-Ayúcar; C. Pennanech; Hasso B. Niemann; Lisa McFarlane; M. R. Leese; Bobby Kazeminejad; G. Israel; B. Hathi; A. Hagermann; J. A. Haberman; Marcello Fulchignoni; Francesca Ferri; Robindro Dutta-Roy; Lyn R. Doose; Jaime E. Demick-Montelara; Giacomo Colombatti
Archive | 2006
Hasso B. Niemann; J. E. Demick; J. A. Haberman; Dan N. Harpold; W. T. Kasprzak; Eric Raaen; S. H. Way; Sushil K. Atreya; G. R. Carignan; Stephen J. Bauer
Archive | 2006
Hasso B. Niemann; Sushil K. Atreya; Jaime E. Demick-Montelara; J. A. Haberman; Dan N. Harpold; W. T. Kasprzak; Tobias Owen; Eric Raaen
Archive | 1998
Hasso B. Niemann; Sushil K. Atreya; G. R. Carignan; T. M. Donahue; J. A. Haberman; D. N. Harpold; R. E. Hartle; D. M. Hunten; W. T. Kasprzak; Paul R. Mahaffy; Tobias Owen; N. W. Spencer