glast large area telescope: instrument design steven m. ritz goddard space flight center
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Gamma-ray Large Area Space Telescope. GLAST Large Area Telescope: Instrument Design Steven M. Ritz Goddard Space Flight Center LAT Instrument Scientist [email protected]. From Science Requirements to Design. From LAT proposal Foldout D:. Simplified Flow. - PowerPoint PPT PresentationTRANSCRIPT
GLAST LAT Project DOE/NASA Review of the GLAST/LAT Project, Feb. 13-15, 2001
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GLAST Large Area Telescope:GLAST Large Area Telescope:
Instrument Design
Steven M. RitzGoddard Space Flight CenterLAT Instrument Scientist
Gamma-ray Large Area Gamma-ray Large Area Space TelescopeSpace Telescope
GLAST LAT Project DOE/NASA Review of the GLAST/LAT Project, Feb. 13-15, 2001
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From Science Requirements to DesignFrom Science Requirements to Design
From LAT proposal Foldout D:
GLAST LAT Project DOE/NASA Review of the GLAST/LAT Project, Feb. 13-15, 2001
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Simplified FlowSimplified Flow
Science Requirements Document (SRD)
LAT LAT Performance Performance SpecificationsSpecifications
Interface Requirements
Document (IRD)
Design Trade Study Space
Mission System Specification (MSS)
LAT Subsystem Requirements
Mission Assurance Requirements (MAR)
GLAST LAT Project DOE/NASA Review of the GLAST/LAT Project, Feb. 13-15, 2001
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LAT Performance SpecificationLAT Performance Specification
The LAT PS sets instrument performance requirements on:– energy range and effective area– energy resolution– single photon angular resolution (68% and 95% containment)– field of view– source location determination– point source sensitivity– single-event time accuracy– background rejection– dead time– gamma-ray source transient detection capabilities on board
The LAT PS also includes the physical, operational and communications requirements.
GLAST LAT Project DOE/NASA Review of the GLAST/LAT Project, Feb. 13-15, 2001
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Experimental TechniqueExperimental Technique• Instrument must measure the direction, energy, and arrival time of high energy photons (from approximately 20 MeV to greater than 300 GeV):
- photon interactions with matter in GLAST energy range dominated by pair conversion: determine photon direction
clear signature for background rejection
e+ e– calorimeter (energy measurement)
particle tracking detectors
conversion foil
anticoincidenceshield
Pair-Conversion Telescope
Energy loss mechanisms:
- limitations on angular resolution (PSF) low E: multiple scattering => many thin layerslow E: multiple scattering => many thin layers high E: hit precision & lever armhigh E: hit precision & lever arm
• must detect -rays with high efficiency and reject the much higher flux (x~104) of background cosmic-rays, etc.;
• energy resolution requires calorimeter of sufficient depth to measure buildup of the EM shower. Segmentation useful for resolution and background rejection.
GLAST LAT Project DOE/NASA Review of the GLAST/LAT Project, Feb. 13-15, 2001
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Some Constraints (MSS & IRD) on InstrumentSome Constraints (MSS & IRD) on Instrument
• Lateral dimension < 1.8m
Restricts the geometric area.
• Mass < 3000 kg
Primarily restricts the total depth of the CAL.
• Power < 650W
Primarily restricts the # of readout channels in the TKR (strip pitch, # layers), and restricts onboard CPU.
• Telemetry bandwidth < 300 kbps orbit average
Sets the required level of onboard background rejection and data volume per event.
• Center-of-gravity constraint restricts instrument height, but a low aspect ratio is already desirable for science.
• Launch loads and other environmental constraints.
GLAST LAT Project DOE/NASA Review of the GLAST/LAT Project, Feb. 13-15, 2001
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Overview of LATOverview of LAT
• 4x4 array of identical towers4x4 array of identical towers Advantages of modular design.
• Precision Si-strip Tracker (TKR) Precision Si-strip Tracker (TKR) Detectors and converters arranged in 18 XY tracking planes. Measure the photon direction.
• Hodoscopic CsI Calorimeter(CAL)Hodoscopic CsI Calorimeter(CAL) Segmented array of CsI(Tl) crystals. Measure the photon energy.
• Segmented Anticoincidence Detector Segmented Anticoincidence Detector (ACD)(ACD) First step in reducing the large background of charged cosmic rays. Segmentation removes self-veto effects at high energy.
• Electronics System Electronics System Includes flexible, highly-efficient, multi-level trigger.
Systems work together to identify and measure the flux of cosmic gamma Systems work together to identify and measure the flux of cosmic gamma rays with energy 20 MeV - >300 GeV.rays with energy 20 MeV - >300 GeV.
GLAST LAT Project DOE/NASA Review of the GLAST/LAT Project, Feb. 13-15, 2001
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Choice of DetectorsChoice of Detectors
• TRACKERsingle-sided silicon strip detectors for hit efficiency, low noise
occupancy, resolution, reliability, readout simplicity.
• CALORIMETER hodoscopic array of CsI(Tl) crystals with photodiode readout
• ANTICOINCIDENCE DETECTORsegmented plastic scintillator tiles with wavelength shifting
fiber/phototube readout for high efficiency and avoidance of ‘backsplash’ self-veto.
for good resolution over large dynamic range; modularity matches TKR; hodoscopic arrangement allows for imaging of showers for leakage corrections and background rejection pattern recognition.
GLAST LAT Project DOE/NASA Review of the GLAST/LAT Project, Feb. 13-15, 2001
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Pre-Proposal Trade Studies SummaryPre-Proposal Trade Studies Summary
GLAST LAT Project DOE/NASA Review of the GLAST/LAT Project, Feb. 13-15, 2001
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Benefits of ModularityBenefits of Modularity
• Construction and Test more manageable, reduce costs and schedule risk.
• Early prototyping and performance tests done on detectors that are full-scale relevant to flight.
• Aids pattern recognition.
• Good match for triggering large-area detector with relatively localized event signatures.
Issue: demonstrate that internal dead areas associated with support material and gaps between towers are not a problem.
Resolution: Detailed Monte-Carlo model of instrument, combined with beam-test data of prototype hardware, used to validate design performance.
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Design Performance Validation: Design Performance Validation: LAT Monte-Carlo ModelLAT Monte-Carlo Model
The current LAT design is based on detailed Monte Carlo simulations.
Two years of work was put into this before any significant investment was made in hardware development.
Cosmic-ray rejection of >105:1 with high gamma ray efficiency. Solid predictions for effective area and resolutions (computer models now verified by beam tests). Current reconstruction algorithms are existence proofs -- many further improvements under development. Practical scheme for triggering.Design optimization.
Simulations and analyses are all OO (C++), based on GISMO toolkit.
Zoom in on a corner of the instrument
First TKR module plane
module walls
scintillators
front scintillators
gaps, dead areas included
The instrument naturally distinguishes most cosmics from gammas, but the details are essential. A full analysis is important.
proton
gamma ray
GLAST LAT Project DOE/NASA Review of the GLAST/LAT Project, Feb. 13-15, 2001
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X Projected Angle3-cm spacing, 4% foils, 100-200 MeV
Data
Monte Carlo
Experimental setup in ESA for tagged photons:
101 102 103 104
Energy (MeV)
0.1
1
10
Con
tain
men
t S
pace
Ang
le (
deg)
68% Containment95% Containment
(errors are 2)
GLAST Data
Monte Carlo
Monte Carlo Modeling Verified inMonte Carlo Modeling Verified inDetailed Beam TestsDetailed Beam Tests
See NIM A446(2000), 444;and SLAC-Pub 8682 (submitted to NIM)
GLAST LAT Project DOE/NASA Review of the GLAST/LAT Project, Feb. 13-15, 2001
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1999-2000 Beam Test at SLAC1999-2000 Beam Test at SLAC
• data system, trigger• hit multiplicities in front and back tracker sections• calorimeter response with prototype electronics.• time-over-threshold in silicon • upper limit on neutron component of ACD backsplash• hadron tagging and first look at response
Using beams of positrons, tagged photons and hadrons, with a ~flight-size tower, studies of
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Beam Test Engineering ModelBeam Test Engineering Model
Flight-scale tower
constructed
• Beam test at SLAC in December 1999
• Balloon flight in 01
CAL and TKR have prototype custom electronics, with all functionality for flight demonstrated.
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• Evolving understanding of the fluxes, new sources of backgrounds included. Right now:
• Work is ongoing: update background fluxes and selections. L1T rate estimate being revised.
Background RejectionBackground Rejection
Source % rate Avg L1T Rate [Hz]
Chime 36 2019
albedo 4 196
Electron 1 30
Albedo p 59 3224
TOTAL 5470
Analysis done thus far for two main reasons:
(1) Necessary for realistic estimate of effective area.
(2) A proof of principle, demonstration of the power of the instrument design.
Capabilities demonstrated.Capabilities demonstrated. Next:Next:Optimize selections. Some science topics may require less stringent background rejections than others.
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Performance PlotsPerformance Plots
Derived performance parameter: high-latitude point source sensitivity (E>100 Derived performance parameter: high-latitude point source sensitivity (E>100 MeV), 2 year all-sky survey: MeV), 2 year all-sky survey: 1.6x101.6x10-9-9 cm cm-2-2 s s-1-1, a factor > 50 better than , a factor > 50 better than
EGRET’s (~1x10EGRET’s (~1x10-7-7 cm cm-2-2ss-1-1).).
(after all background rejection cuts, being updated)
FOV w/ energy measurement due to favorable aspect ratio
Effects of longitudinal shower profiling
GLAST LAT Project DOE/NASA Review of the GLAST/LAT Project, Feb. 13-15, 2001
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Instrument Triggering and Onboard Data FlowInstrument Triggering and Onboard Data Flow
Hardware trigger based on special signals from each tower; initiates readout
Function: • “did anything happen?”
• keep as simple as possible
• TKR 3 x•y pair planes in a row**
workhorse workhorse triggertriggerx
xx
Instrument Total L1T Rate: <5 kHz>
Function: • reject background efficiently & quickly with
loose cuts,
• reduce computing load
• remove any noise triggers
xx
x
• tracker hits ~line up
• track does not point to hit ACD tile
L3T: full instrumentFunction: reduce data to fit within downlink
Total L3T Rate: <30 Hz>
• complete event reconstruction
• signal/bkgd tunable, depending on analysis cuts: cosmic-rays~ 1:1
Spacecraft
OR
(average event size: ~7 kbits)
rates are orbit averaged; peak L1T rate isapproximately 10 kHz. L1T rate estimate being revised. **ACD may be used to throttle this rate, if req.
Upon a L1T, all towers are read out within 20s
Level 1 Trigger
• CAL: LO – independent check on TKR trigger. HI – indicates high energy event ground
Level 2 Processing Level 3 Processing
L2 was motivated by earlier DAQ design that had one processor per tower. Using single-tower info only, background rate reduction was typically a factor 5. On-board filtering hierarchy being redesigned.
On-board science analysis:On-board science analysis: transient detection (AGN
flares, bursts)
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Pre-Proposal Formal Peer ReviewsPre-Proposal Formal Peer Reviews
Subsystem designs and critical technology
development decisions are periodically reviewed
by independent panels that include members
outside of the collaboration.
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Flow into Tracker SubsystemFlow into Tracker Subsystem
-ray conversion efficiencyConverter configuration
Other material
Geometric area
Aspect ratio
Charged particle detection efficiency
Spatial measurement resolutionDead area
Ionization measurementSelf-trigger
Trigger efficiency
Trigger noise rate
Data noise occupancy
Trigger saturation recovery time
Dead time
Total mass
Total power
Environmental
Effective Area
Effective Area Knowledge
Single photon angular resolution requirements
Field of view
Bkgd rejection
Dead time
MSS&IRD requirements
Tel. bndwdth
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-ray conversion efficiencyConverter configuration
Other material
Geometric area
Aspect ratio
Charged particle detection efficiency
Spatial measurement resolutionDead area
Ionization measurementSelf-trigger
Trigger efficiency
Trigger noise rate
Data noise occupancy
Trigger saturation recovery time
Dead time
Total mass
Total power
Environmental
Effective Area
Effective Area Knowledge
Single photon angular resolution requirements
Field of view
Bkgd rejection
Dead time
MSS&IRD requirements
Tel. bndwdth
Flow into Tracker SubsystemFlow into Tracker Subsystem
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Flow into Calorimeter SubsystemFlow into Calorimeter Subsystem
Depth
Geometric area
Passive material
Spatial resolution of energy depositions
Trigger signals
Data noise occupancy
Dynamic range
Total mass
Total power
Environmental
Energy range
Energy resolution
Background rejection
Effective area
Effective area knowledge
Dead time
MSS&IRD requirements
Tel. bndwdth
Measurement dead time
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Flow into ACD SubsystemFlow into ACD Subsystem
Charged particle detection efficiency
Coverage
Maximum false veto due to backsplash
Noise
CNO signals
Trigger signals
Deadtime
Total mass
Total power
Environmental
Energy range
Energy resolution
Background rejection
Effective area
Effective area knowledge
Dead time
MSS&IRD requirements
Tel. bndwdth
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Flow into Electronics SubsystemFlow into Electronics Subsystem
Trigger
Dead/live time measurement
Data flow, deadtime
Command & configuration
Transient analysis and notification
Environmental & Housekeeping data flow
Event filtering
Total mass
Total power
Environmental
Time accuracy
Transient detection and
notification
Energy range
Effective area
Effective area knowledge
Dead time
MSS&IRD requirements
Tel. bndwdth
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Flow into Flight SoftwareFlow into Flight Software
Commanding
Data flow
Monitoring, reporting
Calibration
Event filtering
Transient detection & onboard science analysis
Reprogrammability
Integration and Test
Transient detection and
notification
Energy range
Effective area
Effective area knowledge
Dead time
Tel. bndwdth
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Looking forward to…Looking forward to…