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AbstractAbstract
[en] A gravitational-radiation pulse leaves a unique trace on the Doppler tracking record of a spacecraft. In a one-way microwave link the signal appears twice in the Doppler records. In a link that is transponded (or reflected) from the spacecraft the signal is repeated three times. Similarly some of the sources of Doppler system noise also have a unique, repeated signature. These features provide a meaningful way to improve the sensitivity of proposed spacecraft tracking experiments by using an on-board clock of extremely high stability where the spacecraft and Earth stations each obtain Doppler data. We construct software filters for data from this type of experiment, and using numerical simulations we compare the sensitivity of the proposed new experiments to current ones, where two-way Doppler data are obtained
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Jones, F.C.
National Aeronautics and Space Administration, Greenbelt, MD (USA). Goddard Space Flight Center
National Aeronautics and Space Administration, Greenbelt, MD (USA). Goddard Space Flight Center
AbstractAbstract
[en] The program for the contributed papers contained in Volumes 1 through 8 is presented along with an Author Index for all volumes combined. The confernece program was organized according to three major divisions: (1) Origin and Galactic Phenomena (volumes 1, 2, and 3); (2) Solar and Heliospheric Phenomena (volumes 4 and 5); and (3) High Energy Phenomena (volumes 6, 7, and 8)
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Aug 1985; vp; Available from NTIS, PC A12/MF A01 as TI85015352
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AbstractAbstract
[en] Within the last few years the rapid accumulation of gamma ray burst spectral data, especially those of KONUS and solar maximum mission, has made the confrontation between theories of the gamma ray emission mechanisms and observations much more urgent and challenging. At present the most viable mode seems to be some combination of inverse Comptonization and synchrotron emission. Here, an attempt is made to limit the acceptable parameter space of the emission region by taking into account the maximum set of observational constraints. These are then applied to two specific scenarios: surface emission versus magnetospheric emission. Some observable predictions based on these scenarios are considered
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Source
Jones, F.C.; National Aeronautics and Space Administration, Greenbelt, MD (USA). Goddard Space Flight Center; vp; Aug 1985; vp; Available from NTIS, PC A18/MF A01
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Schwartz, R.A.; Ling, J.C.; Mahoney, W.A.; Wheaton, W.A.; Jacobson, A.S.
Ninteenth International Cosmic Ray Conference. OG sessions, volume 1
Ninteenth International Cosmic Ray Conference. OG sessions, volume 1
AbstractAbstract
[en] The relationship between the hard X-ray and gamma ray emissions during four bursts using the anti-coincidence shields of the High Energy Astronomy Observatory 3 (HEAO 3) Gamma Ray Spectrometer is explored. Recent observations of gamma ray bursts by the Solar Maximum Mission Gamma Ray Spectrometer (GRS) have shown that high energy emission above 1 MeV is a common and energetically important feature (Matz et al. 1985). Time histories of four gamma ray bursts in 3 energy bands ( keV, around 511 keV, and 4 MeV) with 10.24 a resolution show that the 4 MeV flux is only weakly coupled to the spectrum below approximately 600 keV
Primary Subject
Source
Jones, F.C.; National Aeronautics and Space Administration, Greenbelt, MD (USA). Goddard Space Flight Center; vp; Aug 1985; vp; Available from NTIS, PC A18/MF A01
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Fowler, P.H.; Masheder, M.R.W.; Moses, R.T.; Walker, R.N.F.; Worley, A.; Gay, A.M.
Ninteenth International Cosmic Ray Conference. OG sessions, volume 2
Ninteenth International Cosmic Ray Conference. OG sessions, volume 2
AbstractAbstract
[en] For this re-analysis of the Ariel VI data, the contribution of non Z square effects to the restricted energy loss and to Cerenkov radiation in the Bristol sphere has been evaluated using the Mott cross section ratios and the non-relativistic Bloch correction. Results obtained were similar in form to those derived for HEAO3 but with maximum deviations approximately 10% rather than 15% for the Mott term, corresponding to a thinner detector. Because of the large uncertainties in the parameters involved, no relativistic Bloch term was included. In addition the experiments on the HEAO detector make the application of a correction to the Cerenkov response of doubtful justification and none was applied in this analysis. An energy dependent correction was made using an effective energy calculated from the vertical cut-off for a given event. The maximum value of this correction was about 0.6% in Z for low cut-offs, declining to approximately zero by 10 GV
Primary Subject
Source
Jones, F.C.; National Aeronautics and Space Administration, Greenbelt, MD (USA). Goddard Space Flight Center; vp; Aug 1985; vp; Available from NTIS, PC A19/MF A01
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AbstractAbstract
[en] Experiments were carried out on tracks of high energy U ions in olivine, a common meteoritic mineral. The results offer an explanation for the lack of success of previous attempts to derive the Ultraheavy Cosmic Ray composition from the study of tracks in meteorites. They also suggest how such experiments should be performed. The methods tested are described and illustrated
Primary Subject
Source
Jones, F.C.; National Aeronautics and Space Administration, Greenbelt, MD (USA). Goddard Space Flight Center; vp; Aug 1985; vp; Available from NTIS, PC A19/MF A01
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AbstractAbstract
[en] Both the maximum size N sub m and the sea level muon size N sub mu have been used separately to find the all-particle energy spectrum in the air shower domain. However the conversion required, whether from N sub m to E or from N sub mu to E, has customarily been carried out by means of calculations based on an assumed cascase model. It is shown here that by combining present data on N sub m and N sub mu spectra with data on: (1); the energy spectrum of air shower muons and (2) the average width of the electron profile, one can obtain empirical values of the N sub m to E and N sub mu to E conversion factors, and an empirical calorimetric all-particle spectrum, in the energy range 2 x 10 to the 6th power E 2 x 10 to the 9th power GeV
Primary Subject
Source
Jones, F.C.; National Aeronautics and Space Administration, Greenbelt, MD (USA). Goddard Space Flight Center; vp; Aug 1985; vp; Available from NTIS, PC A19/MF A01
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AbstractAbstract
[en] The chemical composition of primary cosmic rays beyond 10 to the 15th power eV could not be measured by the direct method. A more sensitive method to determine the chemical composition is proposed. The method was checked by simulation and compared with existing data on N sub e-N sub mu and N sub e-N sub gamma
Primary Subject
Source
Jones, F.C.; National Aeronautics and Space Administration, Greenbelt, MD (USA). Goddard Space Flight Center; vp; Aug 1985; vp; Available from NTIS, PC A19/MF A01
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Acharya, B.S.; Rao, M.V.S.; Sivaprasad, K.; Sreekantan, B.V.
Ninteenth International Cosmic Ray Conference. OG sessions, volume 2
Ninteenth International Cosmic Ray Conference. OG sessions, volume 2
AbstractAbstract
[en] The size dependence of high energy muons and the size spectrum obtained in the air shower experiment suggest that the mean mass of cosmic rays remains nearly constant at approx 15 up to 5 x 1000,000 GeV and becomes one beyond. The composition model in which nuclei are removed spectrum steepens at 6.7 x 10 power GeV due to leakage from the galaxy, which explains the data which are consistent with data from other experiments
Primary Subject
Source
Jones, F.C.; National Aeronautics and Space Administration, Greenbelt, MD (USA). Goddard Space Flight Center; vp; Aug 1985; vp; Available from NTIS, PC A19/MF A01
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AbstractAbstract
[en] Estimation of the relative intensities of protons and heavy nuclei in primary cosmic rays in the energy region 10 to the 15th power approx. 10 to the 17th power eV, was done by a systematic comparison between all available observed data on various parameters of extensive air showers (EAS) and the results of simulation. The interaction model used is an extrapolation of scaling violation indicated by recent pp collider results. A composition consisting of various percentages of Fe in an otherwise pure proton beam was assumed. Greatest overall consistency between the data and the simulation is found when the Fe fraction is in the region of 25%
Primary Subject
Source
Jones, F.C.; National Aeronautics and Space Administration, Greenbelt, MD (USA). Goddard Space Flight Center; vp; Aug 1985; vp; Available from NTIS, PC A19/MF A01
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