Title: Particle Astrophysics: GLAST
1Particle Astrophysics GLAST
Gamma-ray Large Area Space Telescope
- Peter F. Michelson
- Principal Investigator and Spokesperson, GLAST
LAT Collaboration - Department of Physics SLAC,
- Stanford University
SLAC Scientific Policy Committee Meeting May
12, 2001
2Gamma-ray Large Area Space Telescope
- GLAST Observatory
- spacecraft
- LAT
- GBM
- GLAST Mission
- high-energy gamma-ray
- observatory 2 instruments
- - Large Area Telescope
- (LAT)
- - Gamma-ray Burst
- Monitor (GBM)
- launch (Sept 2005)
- Delta 2 class
- mission operations
- science
- - LAT Collaboration
- - GBM team
- - Guest Observers
- lifetime
- 5 years (minimum)
3Large Area Telescope (LAT)
gt 40 times the sensitivity of EGRET
4GLAST Science Simulated All Sky Map
Virgo Region (E gt 1 GeV)
gt many science objectives
One-Year All-Sky Map (E gt 100 MeV)
5One Year Point Source Catalog
3EG catalog
EGRET 3rd Catalog 271 sources
Expected GLAST LAT 1st Catalog 10,000 sources
6GLAST Science Topics
- Active Galactic Nuclei
- Isotropic Diffuse Background Radiation
- Cosmic Ray Production
- Identify sites and mechanisms
- Endpoints of Stellar Evolution
- Neutron Stars/Pulsars
- Black Holes
- Unidentified Gamma-ray Sources
- Dark Matter
- Solar Physics
- Gamma-Ray Bursts
- DISCOVERY!
7Science capabilities - sensitivity
large field-of-view
200 ? bursts per year ? prompt emission
sampled to gt 20 µs AGN flares gt 2 mn ? time
profile ?E/E ? physics of jets and
acceleration ? bursts delayed emission all
3EG sources 80 new in 2 days ? periodicity
searches (pulsars X-ray binaries) ? pulsar
beam emission vs. luminosity, age, B 104
sources in 1-yr survey ? AGN logN-logS, duty
cycle, emission vs. type, redshift,
aspect angle ? extragalactic background light
(? IR-opt) ? new ? sources (µQSO, ext.
galaxies, clusters)
8International Collaboration
- access to X-ray, MeV, and TeV observatories by
collaboration - for multi-wavelength observations
- mirror data site in Europe
100 collaborators from 28 institutions
CAL
9GLAST LAT Project Recent Upcoming Milestones
- NRC Decadal Astronomy Astrophysics Review ranks
GLAST highest priority moderate-size space
mission for next decade Sept 2000 - 1st joint DOE-NASA Pre-baseline Lehman Review
of GLAST LAT Project Feb 13-15, 2001 - Launch date delayed 6 months due to NASA Mission
funding issues, March 19, 2001 launch now March
2006 - NASA Independent Assessment Review of GLAST
Mission completed in December 2000 recommended
NASA funding augmentation for mission - NASA Headquarters approves IA-recommended mission
funding profile (consistent with March 2006
launch) including contingency funds to procure
Delta II-H (heavy) launch vehicle if needed
April 10, 2001 - LAT Project preparing for DOE-NASA Baseline/PDR
Review this October - Preparing for Balloon Flight of Engineering
Model, Summer 2001 - GLAST LAT Collaboration meeting scheduled for
August 1-2, 2001 at Stanford University
10Status of International Arrangements
- 2 International Agreements and 4 MoAs still being
negotiated complete drafts exist for all
agreements 3 MoAs signed (Japan Sweden UCSC) - International Agreements delayed because
Implementing Arrangement and MoU between DOE and
NASA not in place - International agreements needed with CNES (French
Space Agency) and ASI (Italian Space Agency) - Lack of International Agreement and MoA with
France (CNES) has impacted calorimeter schedule
French team from CEA/Saclay and IN2P3, but
majority of funding from CNES working issues
night day
11GLAST LAT Organization
Collaboration Science Team
E/PO L. Cominsky, SSU
Principal Investigator P. Michelson, SU
SSAC N. Gehrels, GSFC
Instrument Scientist S. Ritz, GSFC
Project Manager W. Althouse, SLAC
Instrument Design Team T. Kamae, SLAC
System Engineer T. Thurston, SLAC
Project Controls T. Boysen, SLAC
Integration Test M. Nordby, SLAC
Electronics DAQ G. Haller, SLAC
Performance Safety Assurance D. Marsh, SLAC
Mech. Systems M. Nordby, SLAC
Sci. Software R. Dubois, SLAC
IOC S. Williams, SU
CAL N. Johnson, NRL France, Sweden
TKR R. Johnson, UCSC SLAC, Italy, Japan
ACD J. Ormes, GSFC
12Collaboration Organization
- Senior Scientist Advisory Committee
- N. Gehrels, Chair
- P. Michelson, PI/Spokesperson
- G. Barbiellini, Italy
- R. Bellazzini, Italy
- E. Bloom, U.S.
- T. Burnett, U.S.
- P. Carlson, Sweden
- A. Djannati-Atai, France
- R. Dubois, U.S.
- Advises PI/Spokesperson on science issues and
science organization of collaboration - Implements collaboration membership policy and
publication policy - Meets quarterly
- I. Grenier, France
- N. Johnson, U.S.
- R. Johnson, U.S.
- T. Kamae, Japan
- J. Ormes, U.S.
- S. Ritz, U.S.
- H. Sadrozinski, U.S.
- D. Thompson, U.S.
- K. Wood, U.S.
13Collaboration Organization
- Instrument Design Team
- Chaired by Instrument Technical Manager, T. Kamae
- Deputy Chairs R. Bellazzini (Italy), E. Bloom
(US), J. Paul (France) - Reports to Project Manager, W. Althouse
- Forum for exchange of information between
subsystems to maintain coordinated design
resolve issues or refer to IPO for resolution - Membership includes all subsystem managers key
system engineering personnel - IDT members obliged to attend IDT meetings
meetings open to the Collaboration - Weekly video conference meetings
14GLAST Mission Science Working Group
- Advises the GLAST Mission Project on matters
related to the scientific development of the
GLAST mission - Jonathan Ormes, Chair, GLAST Mission Project
Scientist - Guido Barbiellini, Italy
- Elliott Bloom, USA
- Patrizia Caraveo, Italy
- Charles Dermer, (IDS), USA
- Brenda Dingus, (IDS), USA
- Neil Gehrels, Deputy Proj. Scientist, USA
- Isabelle Grenier, France
- Neil Johnson, USA
- Tuneyoshi Kamae, Japan
- Giselher Lichti, (GBM), Germany
Charles Meegan, (PI-GBM), USA Peter Michelson,
(PI-LAT), USA M. Pohl, (IDS), Germany David
Thompson, USA Steve Thorsett, (IDS), USA Steve
Ritz, Deputy Project Sci., USA Lynn Cominsky,
E/PO Don Kniffen, ex officio, Program Scientist
GLAST LAT Collaboration Members
15GLAST Large Area Telescope (LAT) Design
Instrument
Pair-conversion telescope
Instrument must measure the direction, energy,
and arrival time of high-energy photons (20 MeV -
gt300 GeV)
- energy resolution requires calorimeter depth
sufficient to measure buildup of EM shower. - calorimeter segmentation useful for
resolution - background rejection
16Large Area Telescope (LAT) Design Overview
Instrument
16 towers ? modularity height/width 0.4 ?
large field-of-view Si-strip detectors total
of 106 ch. hodoscopic CsI crystal array
? cosmic-ray rejection ? shower
leakage correction shower max
contained lt 100 GeV segmented plastic
scintillator ? minimize self-veto
Tracker
Calorimeter
Anticoincidence Detector Shield
3000 kg, 650 W (allocation) 1.75 m ? 1.75 m ?
1.0 m 20 MeV 300 GeV
Flight Hardware Spares 16 Tracker Flight
Modules 2 spares 16 Calorimeter Modules 2
spares 1 Flight Anticoincidence Detector Data
Acquisition Electronics Flight Software
17GLAST Large Area Telescope (LAT) Design
Tracker Modules
Si-strip detectors fine pitch 228 mm, high
efficiency 12 front tracking planes (x,y) 3
x 12 0.45 Xo reduce multiple
scattering 4 back tracking planes (x,y)
18 x 4 0.72 Xo increase
sensitivity gt 1 GeV
e
e
18GLAST Large Area Telescope (LAT) Design
Calorimeter Modules
Hodoscopic Imaging Array of CsI crystals
8.5 rl depth PIN photodiode readout from both
ends 2 ch/xtal x 96 xtals/mod 2,944 ch
segmentation allows pattern
recognition (imaging) and
leakage correction
Mechanical Prototype of Carbon Cell Design
19GLAST Large Area Telescope (LAT) Design
Anticoincidence Shield
Segmented, plastic scintillator tile array
high efficiency, low-noise, hermetic
segment ACD sufficiently and
only veto event if a track points to
hit tile
ACD tile readout with Wavelength Shifting Fiber
20Detector Performance Verified in Detailed Beam
Tests
21PSF measured for Flight-scale Prototype Tracker
22Energy Response measured for Flight-scale
Prototype Calorimeter Module
23The PSF as a function of the reconstructed energy
for data and Monte Carlo simulation. The expected
1/E behavior is clearly seen. As the photon
energy increases, multiple scattering becomes
less important and the PSF decreases. At high
energies the point spread function is dominated
by the finite spatial resolution of the silicon
detectors (60 microns). The thick radiators at
the back of the tracker widen the point spread
function by slightly more than a factor of 2.
24Because of the calorimeter depth, the shower
maximum is contained up to 50 GeV at normal
incidence. However, above a few GeV, a large
amount of energy leaks out the back of the
calorimeter, and the total energy measured is
systematically less than the incident energy. We
have employed two techniques to correct for the
shower leakage. We show the raw and reconstructed
energy for 20 GeV incident positrons. The
resolution of the raw distribution is around 7,
while the reconstructed resolution is less than
4 by the correlation method and about 5 by
profile fitting. The reconstruction method
applied to Monte Carlo simulated data yields an
energy resolution of 3, suggesting that some
uncertainties remain in our calibration of beam
test data.
25Schedule