~ _- IDOCLRXKT DMSP SATELLITE DETECTIONS OF GAMMA-RAY BURSTS. J. Terrell, NIS-2 P. Lee, NIS-2 R W.

Similar documents
CQNl_" RESPONSE TO 100% INTERNAL QUANTUM EFFICIENCY SILICON PHOTODIODES TO LOW ENERGY ELECTRONS AND IONS

Data Comparisons Y-12 West Tower Data

Applications of Pulse Shape Analysis to HPGe Gamma-Ray Detectors

Use of Gamma Rays from the Decay of 13.8-sec "Be to Calibrate a Germanium Gamma Ray Detector for Measurements up to 8 MeV

Ray M. Stringfield Robert J. Kares J. R. Thomas, Jr.

Hyperon Particle Physics at JHF. R. E. Mischke

A Few-Group Delayed Neutron Model Based on a Consistent Set of Decay Constants. Joann M. Campbell Gregory D. Spriggs

ION EXCHANGE SEPARATION OF PLUTONIUM AND GALLIUM (1) Resource and Inventory Requirements, (2) Waste, Emissions, and Effluent, and (3) Facility Size

PROJECT PROGRESS REPORT (03/lfi?lfibr-~/15/1998):

Optimization of NSLS-II Blade X-ray Beam Position Monitors: from Photoemission type to Diamond Detector. P. Ilinski

Cosmological Gamma-Ray Bursts. Edward Fenimore, NIS-2 Richard Epstein, NIS-2 Cheng Ho, NIS-2 Johannes Intzand, NIS-2

12/16/95-3/15/96 PERIOD MULTI-PARAMETER ON-LINE COAL BULK ANALYSIS. 2, 1. Thermal Neutron Flux in Coal: New Coal Container Geometry

Abstract of paper proposed for the American Nuclear Society 1997 Winter Meeting Albuquerque, New Mexico November 16-20, 1997

Development of a High Intensity EBIT for Basic and Applied Science

(4) How do you develop an optimal signal detection technique from the knowledge of

0STI. E. Hammerberg, XNH MD SIMULATIONS OF DUSTY PLASMA CRYSTAL FORMATION: PRELIMINARY RESULTS M. J. S. Murillo, XPA

Plutonium 239 Equivalency Calculations

IMAGING OF HETEROGENEOUS MATERIALS BY. P. Staples, T. H. Prettyman, and J. Lestone

SPHERICAL COMPRESSION OF A MAGNETIC FIELD. C. M. Fowler DISCLAIMER

Turbulent Scaling in Fluids. Robert Ecke, MST-10 Ning Li, MST-10 Shi-Yi Li, T-13 Yuanming Liu, MST-10

Using the X-FEL to understand X-ray Thomson scattering for partially ionized plasmas

Further Investigation of Spectral Temperature Feedbacks. Drew E. Kornreich TSA-7, M S F609

How Small Can a Launch Vehicle Be?

ust/ aphysics Division, Argonne National Laboratory, Argonne, Illinois 60439, USA

Walter P. Lysenko John D. Gilpatrick Martin E. Schulze LINAC '98 XIX INTERNATIONAL CONFERENCE CHICAGO, IL AUGUST 23-28,1998

MULTIGROUP BOLTZMANN FOKKER PLANCK ELECTRON-PHOTON TRANSPORT CAPABILITY IN M C N P ~ ~ DISCLAIMER

Alamos National Laboratory is operated by the University of California for the United States Department of Energy under contract W-7405-ENG-36

Roger J. Bartlett, P-22 Dane V. Morgan, P-22 M. Sagurton, EG&G J. A. Samson, University of Nebraska

Los Alamos IMPROVED INTRA-SPECIES COLLISION MODELS FOR PIC SIMULATIONS. Michael E. Jones, XPA Don S. Lemons, XPA & Bethel College Dan Winske, XPA

Analysis of Shane Telescope Aberration and After Collimation

TOWARDS EVEN AND ODD SQUEEZED NUMBER STATES NIETO, MICHAEL M

Alex Dombos Michigan State University Nuclear and Particle Physics

Plasma Response Control Using Advanced Feedback Techniques

A Germanium Detector with Optimized Compton Veto for High Sensitivity at Low Energy

Response to Comment on "The National Ignition Facility Laser Performance Status"

S.A. Kreek J.E. Kammeraad D. Beckedahl G.J. Schmid J.J. Blair B. Payne A. Friensehner

Excitations of the transversely polarized spin density. waves in chromium. E3-r 1s

Magnetic Measurements of the Elliptical Multipole Wiggler Prototype

Start-up Noise in 3-D Self-AmpMed

A TER. Observation of Xe with the PNNL ARSA System PNNL UC-7 13

Three-Dimensional Silicon Photonic Crystals

Modeling Laser and e-beam Generated Plasma-Plume Experiments Using LASNEX

DML and Foil Measurements of ETA Beam Radius

Fission-Fusion Neutron Source

National Accelerator Laboratory

Partial Discharge Characterization of High-Voltage Cables and Components

UPGRADED CALIBRATIONS OF THE THOMSON SYSTEM AT DIII D

Los Alamos. OF nm LA-"'- Title: HYBRID KED/XRF MEASUREMENT OF MINOR ACTINIDES IN REPROCESSING PLANTS. S. T. Hsue and M. L.

RESEARCH OPPORTUNITIES AT THE CNS (Y-12 AND PANTEX) NUCLEAR DETECTION AND SENSOR TESTING CENTERS (NDSTC)

Lawrence Berkeley National Laboratory Lawrence Berkeley National Laboratory

August 3,1999. Stiffness and Strength Properties for Basic Sandwich Material Core Types UCRL-JC B. Kim, R.M. Christensen.

Tell uric prof i 1 es across the Darrough Known Geothermal Resource Area, Nevada. Harold Kaufniann. Open-file Report No.

BASAL CAMBRIAN BASELINE GEOLOGICAL CHARACTERIZATION COMPLETED

The Radiological Hazard of Plutonium Isotopes and Specific Plutonium Mixtures

Summary Report: Working Group 5 on Electron Beam-Driven Plasma and Structure Based Acceleration Concepts

AuttWr(s): A. Blotz, Theoretical Division, Los Alamos National Laboratory, Los Alamos, NM 87545, USA

Multi-Scale Chemical Process Modeling with Bayesian Nonparametric Regression

GA A23736 EFFECTS OF CROSS-SECTION SHAPE ON L MODE AND H MODE ENERGY TRANSPORT

Experiment. The Pinhole Neutron. Pinex. c. c. sartain UCRL-ID November 21,1958

GA A22677 THERMAL ANALYSIS AND TESTING FOR DIII D OHMIC HEATING COIL

Quarterly Report April 1 - June 30, By: Shirley P. Dutton. Work Performed Under Contract No.: DE-FC22-95BC14936

PROJECT PROGRESS REPORT (06/16/1998-9/15/1998):

Measurement of Low Levels of Alpha in 99M0Product Solutions

BWXT Y-12 Y-12. A BWXT/Bechtel Enterprise SMALL, PORTABLE, LIGHTWEIGHT DT NEUTRON GENERATOR FOR USE WITH NMIS

National Accelerator Laboratory

The temperature dependence of the C1+ propylene rate coefficient and the Arrhenius fit are shown in Figure 1.

AEC Research and Development REPORT

Use of AVHRR-Derived Spectral Reflectances to Estimate Surface Albedo across the Southern Great Plains Cloud and Radiation Testbed (CART) Site

FUSION TECHNOLOGY INSTITUTE

AC dipole based optics measurement and correction at RHIC

SciDAC CENTER FOR SIMULATION OF WAVE-PLASMA INTERACTIONS

A NEW TARGET CONCEPT FOR PROTON ACCELERATOR DRIVEN BORON NEUTRON CAPTURE THERAPY APPLICATIONS* Brookhaven National Laboratory. P.O.

4kU. Measurement of Storage Ring Motion at the Advanced Light Source. QSTt ERNESTORLANDO LAWRENCE BERKELEYNATIONAL LABORATORY

Cable Tracking System Proposal. Nick Friedman Experimenta1 Facilities Division. June 25,1993. Advanced Photon Source Argonne National Laboratory

GA A22722 CENTRAL THOMSON SCATTERING UPGRADE ON DIII D

GA A26474 SYNERGY IN TWO-FREQUENCY FAST WAVE CYCLOTRON HARMONIC ABSORPTION IN DIII-D

PLASMA MASS DENSITY, SPECIES MIX AND FLUCTUATION DIAGNOSTICS USING FAST ALFVEN WAVE

A Distributed Radiator, Heavy Ion Driven Inertial Confinement Fusion Target with Realistic, Multibeam Illumination Geometry

: Y/LB-16,056 OAK RIDGE Y-12 PLANT

in the pinch. This paper describes the computer modeling behind the shielding design of a

RUDOLPH J. HENNINGER, XHM PAUL J. MAUDLIN, T-3 ERIC N. HARSTAD, T-3

Peak Reliability Delivering near real-time phase angle deltas using Inter-Control Center Communication Protocol (ICCP)

8STATISTICAL ANALYSIS OF HIGH EXPLOSIVE DETONATION DATA. Beckman, Fernandez, Ramsay, and Wendelberger DRAFT 5/10/98 1.

SOLAR SEMIDIURNAL TIDAL WIND OSCILLATIONS ABOVE THE CART SITE. Prepared for the U.S. Department of Energy under Contract DE-AC06-76RLO 1830

GA A27806 TURBULENCE BEHAVIOR AND TRANSPORT RESPONSE APPROACHING BURNING PLASMA RELEVANT PARAMETERS

Multi-scale modeling with generalized dynamic discrepancy

Modeling of psec-laser-driven Ne-like and Ni-like X-ray lasers. Joseph Nilsen

PROGRESS REPORT JULY TO SEPTEMBER

APPLICATION SINGLE ION ACTIVITY COEFFICIENTS TO DETERMINE SOLVENT EXTRACTION MECHANISM FOR COMPONENTS OF NUCLEAR WASTE

GA A26057 DEMONSTRATION OF ITER OPERATIONAL SCENARIOS ON DIII-D

On the HalfiLife of LABORATORY ERNEST ORLANDO LAWRENCE BERKELEYNATIONAL. and Particle Astrophysics Nuclear Science and Physics Divisions

Direct Determination of the Stacking Order in Gd 2 O 3 Epi-Layers on GaAs

sample-specific X-ray speckle contrast variation at absorption edges $ & ~ 0

RECEIVED SEQ

Variational Nodal PerturbationCalculations Using Simplified Spherical HarmonicsO

Flipping Bits in the James Webb Space Telescope s Cameras

ASTER CONF-~W OSTI MAY DISTRIBUTION OF THIS

LUMINOSITY REQUIREMENTS FOR HIGGS RESONANCE STUDIES AT THE FIRST MUON COLLIDER*

Two-Screen Method for Determining Electron Beam Energy and Deflection from Laser Wakefield Acceleration

DETECTING AND QUANTIFYING LEWISITE DEGRADATION PRODUCTS I N ENVIRONMENTAL SAMPLES USING ARSENIC SPECIATION*

Transcription:

TITLE: AUTHOR(S): SUBMITTED TO: DMSP SATELLITE DETECTIONS OF GAMMARAY BURSTS J. Terrell, NIS2 P. Lee, NIS2 R W. Klebesadel, NIS2 Huntsville GRB Symposium Proceddings, Huntsville, AL NATIONAL LABORATORY b s Alamos National Laboratory, an affirmativeactiordequal opportunity employer. is operated by the University of California for the U.S. Department of Energy under contract W745ENG36. By acceptance of this article, the publisher recognizes that the U.S. Government retains a nonexclusive, royanyfree license to publish or reproduce the published form of thls contribution, or to allow others lo do so, for U.S. Government purposes. The Los Alamos National Laboratory requests that the publisher identify this article as work performed under the auspices of the U.S. Deparlment of Energy. Form No. 836 R5 ~ I ~ OF ~ IDOCLRXKT ~ ~1s @U:fslTELI ~ ' TD k ~ _ ~ ~ ST2629 I N 1

DMSP Satellite Detections of GammaRay Bursts I 1 J. Terra, P. Lee, and R W. Klebesadel Los Alamos National Laboratory J. W. Griffe Sandia National Laboratory Gammaray burst detectors are aboard six U. S. Air Force Defense Meteorological Satellite Program (DMSP) spacecraft, two of which are currently in use. Their 8km altitude orbits give a field of view to 117" from the zenith. A great m y bursts have been detected, usually in coincidence with detections by GRO or other satellites such as PVO or ULYSSES. The directions of the sources can be determined with considerable accuracy from such correlated observations, even when GF?D/BATSE with its directional capabilities is not involved. Thus these DMSP data, especially in conjunction with other observations, should be helpful in trying to understand the true nature of gammaray bursts. INTRODUC'J?CON Six of the DMSP spacecraft launched by the U. S. Air Force have carried gamm+ray burst detectors into orbit at 8 km. Two of these (DMSP 12 and 13) are currently in operation, in nearpolar orbits, attaining latitudes of 81' with an initial launch direction of 99'. Each carries two gammaray detectors with ~ 1 cm2 of NaI, sensitive to gammarays of 5 kev or more coming from sources within ~ 1 1 7 'of the spacecraft zenith. A fuller description may be found el~ewherel~. RESULTS Many gammaray bursts have been detected by two or more of the DMSP spacecraft. When other spacecraft have also detected these bursts, relative times of detection and fields of view can give considerable information on source location, even when no detection was made by the Compton Observatory (GRO). Such a burst was detected by DMSP 11, 12, and 13 on 7 April 1995, and also by ULYSSES and WIND. Figure 1shows the data from DMSP 11for this @ 1996 American Institute of Physics 1

DMSPll 16 1995 APR 7 yl 9597 C1L CIS ClU CIH CIU C2L C2S C2U C2H CZU y..ou t u w. 6 u.8 1.. I... p.u DZs (..e e.. OUI u.. u.rg547g..i.*a.1.*95129 14 12 n 1 z w s a I 3 z 6 4 2 2 4 6 8 1 12 14 TIME (SECONDS AFTER 5 4 9 ) 16 18 2 FIG. 1. DMSP 11data for a hard gammaray burst on 7 April 1995. hard burst, with gamma rays exceeding 43 kev in both detectors (for DMSP 11 the channel thresholds are at 5, 1, 2, 43, and 55 kev, with cutoff at 1 kev). The first countingrate peak in the DMSP data occurred in the 2second time channel centered on 54932 sec UT. Direction analysis, undertaken in cooperation with other investigators, has not yet been completed for this and other events reported here. Another hard burst, much more intense, was detected on 22 August 1995. The DMSP 12 data are shown in Figure 2. This was probably the most intense burst ever detected by DMSP satellites, with a counting rate increasing to almost 4 counts/sec at the peak time of 13767 sec UT. It was also detected by BATSE (GRB No. 3767), KONUS, and ULYSSES. DMSP 13 detected a softer but interesting burst on 25 August 1995, shown in Figure 3. The first peak count at 15786 sec UT was followed by a brief higher peak at 15864 sec, and then by a long highenergy peak extending from ~ 1 5 9 to 1695 sec UT. The NaI detectors on DMSP 13 have thresholds at 6, 15, 375 kev. The highenergy peak (lowest counting rates in Figure 2) corresponds to photons of energy >6 MeV. One of the strongest bursts ever detected by BATSE and COMPTEL4j5 was GRB No. 2831 ("Olympic"), which triggered BATSE at 82962 sec U T on 17 February 1994. This was also detected by DMSP 1, DMSP 11, and ULYSSES. The data from DMSP 1, shown in Figure 4, indicate a curious pattern of repeated outbursts over ~ 1 8 seconds. A Fourier analysis of this

TIME (SECONDS AFTER 1 3 7 ) FIG. 2. DMSP 12 data for a hard and very intense gammaray burst on 22 August 1995. 2 o so IW IM zoo 25. aw TIME (SECONDS AFTER 157) as 4w FIG. 3. DMSP 13 data for a soft gammaray burst followed by a very long hard afterpulse, on 22 August 1995.

TIME (SECONDS AFTER 829) FIG. 4. DMSP 1 data for the intense gammaray burst of 17 February 1994. data (that corresponding to the highest counting rates) gives some evidence of a periodicity of ~ 2 seconds 4 (Figure 5); the same result is given by DMSP 11 data. Thus it is possible that this gammaray burst has a pulsating character reminiscent of the 5 March 1979 burst with its 8sec periodicity6. However, the fact that the length of the outburst is only about seven periods necessarily means that the evidence for periodicity is uncertain. Randomly occurring "shot noise" (1sec pulses) can give a similar Fourier spectrum, with maximum power near zero frequency7js. Considering that each point in Figure 5 has a standard deviation of 196, or 5% even when smoothed over 4 terms, the power spectrum gives no conclusive evidence of periodicity. CONCLUSIONS The DMSP spacecraft have produced a large body of data on gammaray bursts, representing a considerable resource for the study of these events. The data include time histories and spectral information, and directional information can be greatly enhanced by combining these observations with those of other spacecraft. They may well be of service in obtaining a fuller understanding of the origin of gammaray bursts.. This work was supported by NASA, by the U. S. Department of Defense, and by the U. S. Department of Energy. DISCLAIMER This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof.

AVC. 716.1647 VAR 165SOO.4 24 5 22OW 2 18 16 14 ' z f 12WO 2 'low 8Ooa 6oW 4WO 2.2.OO.4.6.8.IO.I2.I4.16.18 FREQUENCY (HERTZ) G2LOUH S 95129 UT 85 OF.588 I t.2 22 2 4 2 6 2.ooOo ( S E W S ) FIG. 5. Fourier power spectrum of the gammaray burst data in Figure 4 (DMSP 1, 17 February 1994). 1. J. Terrell, P. Lee, R W.Klebesadel, and J. W. Griffe, in GammaRay Bursts, AIP Conference Proceedings 265, p.48 (AIP, New York, 1992). 2. J. Terrell, P. Lee, R W. K l e b d e l, and J. W. Griffe, in Compton GammaRay Observatory, AIP Conference Proceedings 28,p.788 (AIP, New York, 1993). 3. J. Terrell, P. Lee, R W.Klebesadel, and J. W. Griffe, in GammaRay Bursts, AIP Conference Proceedings 37,p.34 (AIP, New York, 1994). 4. R M. Kippen et al., M U Circular No. 5937 (21 February 1994). 5. IC Hurley et al., Nature 372, 652 (1994). 6. J. Terrell, W. D. Evans, R W. K l e b d e l, and J. G. Larm, Nature 285, 383 (198). 7. J. Terrell and K. H. Olsen, Astrophysical J. 161, 399 (197). 8. N. J. Terrell, Astrophysical J. 174, L35 (1972)...