PSI’s Space Radiation Instrumentation Radiation Detection & Dosimetry 6-7 April 2006 G. E. Galica Physical Sciences Inc. 20 New England Business Center Andover, MA 01810-1077 www.psicorp.com Slide 2 PSI Rad Sensor Experience • PSI has developed several generations of charged particle sensors – Space science – Spacecraft & microelectronics survivability – Spacecraft operations support • SDOM [JAXA] – Gen1 – 1-200 MeV protons, 0.5-10 MeV electrons, alphas, Heavy ions - 32 particle-energy bins – 2 sensors currently flying (GEO & GTO), 1 awaiting launch on JEM • LPD [USEF(Japan)] – Gen2 – 1-150 MeV protons, 0.3-20 MeV electrons, alphas/heavy ions - 12 particle-energy bins – 1 sensor currently flying (1000 km polar), follow-on sensor launch 2007 • CEM [NASA LWS SET] – Gen2 – Modified LPD – Launch 2009 • HIPS [AFRL] – Gen3 – LPD derivative – High energy electrons and protons, Imaging sensor – Development started (launch 2009 on DSX) • LIPS [AFRL] – 20-2000 keV protons and electrons – Imaging sensor, 12 energy bins x 8 angular bins – Launch 2009 on DSX • PSI has flown > 20 instrument and experiments since 1991 on satellites, shuttle and space station Slide 3 PSI Rad Sensor Design Objectives & Data Quality • PSI GEN1& GEN2 radiation sensors had several performance goals that have now been demonstrated on orbit: • Single sensor to detect protons, electrons, alphas, heavy ions • Large throughput (A omaga) – up to 0.3 cm2 sr – Results in high count rates, efficient detection of small populations of particles, good counting statistics • High count rate – up to 200 kcps – Does not saturate during solar storms • Good particle discrimination – Cross-contamination between electrons and protons can be a significant problem – SDOM & LPD (GEN1&2 sensors) achieved <10 to the -4 contamination – Achieved through sensor design and on-board processing • High accuracy calibration and validated sensor model – Returning fully calibrated data from sensor turn-on • Flight proven technology on multiple orbital missions • High quality, calibrated data received from turn-on Slide 4 LPD – Light Particle Detector (GEN-2) • Designed for and flying on the SERVIS-1 satellite (Japan) – Space Environment Reliability Verification Integrated System – Orbital mission Oct03-present – SERVIS-2 follow-on launch 2007 – CEM for LWS-SET • Baseline Energy Range – protons: 1 to 150 MeV (6 bins) – electrons: 0.3 to 10 MeV (4 bins) – alphas: >12 MeV (1 bin) – ions: >3 MeV/nucleon (1 bin) • Large G-factor/high count rate – 0.2 cm2sr – 200 kcps • FPGA-based processing • Extensive ground calibration & modeling • Physical parameters – 4 kg (fully redundant) – 7 W (HiRel/RadHard) image of Gen-2 Light Particle detector Slide 5 Generic Block Diagram • Combination of multiple detectors: SSDs and scintillator • AntiCoincidence Scintillator rejects side penetrating particles • Collimator defines acceptance angle for low energy particles • High-speed analog circuitry and ADC (12-bit) enables 200 kcps rate • High-speed, FPGA-based processor reduces data volume Generic Block Diagram with labels: Collimator, Foil Window, SSD1, SSD2, Anti-Coincidence Scintillator Passive Shielding, CSP/Peahold, Calibration Telemetry Drivers, S/C Telemetry, DC/DC Converter, Filter, S/C Power. FPGA - Event Detection - Particle Type - Energy Analysis - Binning - Spacecraft Interface Slide 6 Modeling and Calibration • All PSI sensors are modeled using the GEANT4 code – no free parameters • The model is validated with calibration data – Sensors are calibrated over nearly their entire particle-energy range • We use the model to: – develop and refine the sensor and algorithm design – interpolate/extrapolate sensor response to uncalibrated regimes – predict on-orbit performance – interpret orbital data diagram of SERVIS with label 10 MeV electrons graph of Proton Scintillator Respnse with proton energy range 0 - 160 MeV Slide 7 Sensor Calibration & Modeling • PSI extensively calibrates its radiation sensors – over nearly their entire particle / energy ranges • We develop full 3D sensor models to describe performance – GEANT4 based models – No free parameters • We validate the models with ground calibration data • Use the models for to interpolate and extrapolate sensor performance uncalibrated regions – Design phase – Interpretation of orbital data Particle Energy (MeV) Facility Proton 0.03-1.0 UNT 0.9-1.7 NASA GSFC 7.5-31 Yale Wright NSL 15-225 NPTC 50-250 IUCF Electron 0.03-0.4 NIST C-W 0.5-2.0 NIST VdG 7-32 NIST MIRF Alpha 10-50 Yale Wright NSL Ion (C) 15-120 Yale Wright NSL Slide 8 SERVIS LPD – 2 Dec 03 • On 2 Dec 2003, SERVIS LPD detected a sudden, spatially distinct enhancement of low-energy protons • Low energy protons (1 to 12 MeV) enhanced first • Enhancement in higher energy protons (12 to 25 MeV; 25 to 50 MeV) occurred after a delay • Small changes in electron activity • SAA proton flux was also enhanced graph of protons - 2 Dec 03 with axis Flux (cm-2 s-1) with range 1.E+01 to 1.E+07 to UT (hh:mm) with range 8:00 to 20:00 labels p1 - 1.5-12 MeV, p2 - 13-25 MeV, p3 - 25-37 MeV, p4 - 38 - 53 MeV, p5 - 53-96 MeV, p6 - 96-150 MeV graph of electrons - 2 Dec 03 with axis Flux (cm-2 s-1) with range 1.E+01 to 1.E+07 to UT (hh:mm) with range 8:00 to 20:00 labels e1 - 0.3-1.5 MeV, e2 - 1.7-3.4 MeV, e3 - 3.4-636 MeV, e4 - >6.6 MeV Slide 9 Electron / Proton contamination • LPD and SDOM both exhibit very small amounts of contamination by low energy electrons • <10 to the -4 contamination of low-energy protons by electrons graph of Electon / Proton contamination 1000 km, 98 deg, 01Dec03 axis labels bin counts with range 1.E+00 to 1.E+06 to time (hh:mm) with range 9:20 to 10:20 electrons (0.3-1 MeV) protons (1-10 MeV) SERVIS-1 LPD Slide 10 SDOM – Standard Dose Monitor (GEN-1) • PSI and MELCO developed a charged particle spectrometer • Delivered 3 flight units for NASDA (Japan) satellites – MDS1: GTO – DRTS: GEO – JEM: LEO • Characterizes the higher energy orbital radiation environment – protons: 1 to 200 MeV, 12 bins – electrons: 0.4 to 20 MeV,5 bins – alphas: 7 to 150 MeV, 4 bins – ions: >1.5 MeV/nucleon • High count rate • Excellent rejection of Lo-E electrons Image of inside an outside of Gen-1 Slide 11 MDS1 SDOM Data • Two SDOM units currently on orbit – MDS1: GTO – DRTS: GEO • PSI involved in orbital data analysis • Currently 3 years of DRTS data; 27 months of MDS1 data Proton Spectr - 22 May 2002 graph of Flux (prot/cm2/sr/sec/Mev) to Time (UT) labels for -0.9-1.1 MeV, - 1.1-1.5 MeV, - 1.5-2.0 MeV, - 2.0-2.7 MeV, - 2.7-3.7 MeV, -3.7-5.4 MeV, -5.7-8.0 MeV, -7-15 MeV, -11-26 MeV, -22-44 MeV, -40-80 MeV, -90-200 MeV Electron Spectr - 22 May 2002 graph of Flux (elect/cm2/sr/sec/Mev) to Time (UT) labels for -0.4-.09 MeV, - 0.9-2.0 MeV, - 1.7-5.0 MeV, - 6-11 MeV, - 10-20 MeV Alpha/ion Spectr - 22 May 2002 graph of Flux (part/cm2/sr/sec/Mev) to Time (UT) labels for A - 6.5-12 MeV, A - 13-24 MeV, A - 25-52 MeV, A - 76-144 MeV, H - >1.5 MeV/nucl Slide 12 DRTS SDOM – GOES Intercomparison • Compared DRTS-SDOM data to GOES data for complete Oct/Nov 2003 Flare – Start time: 25 Oct 2003 15:06:43 – End time: 13 Nov 2003 15:27:42 • Mapped SDOM bins onto GOES bins – Sum over SDOM energy bins – Time average SDOM data • Quantitative comparison between GOES and SDOM is quite good • SDOM not saturated during flare • SDOM low-energy electron bins not contaminated by high energy protons • SDOM provides better energy and temporal resolution graph for Flare 12 25-Oct-2003 15:06:43 to 13-Nov-2003 15:27:42 Axis values Flux (1.m2-sr sec) with range 10 to the -2 to 10 to the 6th power and Time Labels for GOES data and ave SDCM data, p+ > 5 MeV graph for Flare SDOM A6 & GOES A4+A5 25-Oct-2003 15:06:43 to 13-Nov-2003 15:27:42 Axis values Flux (1.m2-sr sec) with range 10 to the -2 to 10 to the 6th power and Time Labels for GOES data and ave SDCM data, A - 60-250 MeV Slide 13 DSX HIPS (GEN-3) design of DSX HIPS (Gen-3) with labels for SSDs, scint, B-Field, collimator, ACS, PCBs • High-energy Imaging Particle Spectrometer – Under development for AFRL –DSX mission (COTR: M. Golightly) – Currently in EM phase – 2007 delivery; 2009 launch • Energy Range – Protons 10 - 300 MeV (8 bins) – Electrons 0.5 - 30 MeV (12 bins) • Pitch angle distribution measurement – 7 x 90 deg FOV – 16 pixels • Physical – 200 x 210 x 120 mm3 – 10.5 W–5 kg – 740 bytes/sec Slide 14 Modular Configuration • LPD is designed around flight-proven detector and electronics modules • Modular design enables rapid development of new sensors – alter energy ranges by changing detectors – alter bin configuration • Working bench model enables rapid prototyping, calibration and validation of new designs • Redundant and non-configurations available • Easily configure systems image of Modular Configuration with labels for SSD, PMT, SSD-HV PMT-HV, Power, Digital-B , Digital-A, H-0095 Slide 15 LPD Modules Image of LPD Modules with labels for Telescope, SSD A&B, Scintillator, PMT-HV, SSD Board, PMT Board SSD-HV image of LPD Modules with labels SSD Module, and Scintillator Module Slide 16 Reconfiguration of Redundant Systems • EM modular processors available for rapid prototyping • We create a sensor with greater capability by reconfiguring the basic redundant system • 2 detectors - 3 detectors • 1 processor - 2 processors PSI PROPRIETARY design of SERVIS LPD and WINDS Option 2 for reconfiguration of redundant systems. Labels for Collimator, Window, SERVIS LPD SSd Board, HV SERVIS LPD PMT Board, Scintillator, SSD-1, SSD-2, HV, CSP, SERVIS LPD Digital-B, SERVIS LPD Digital-A, DAE TLM, DAE Power and DAE TLM Slide 17 Advanced Radiation Shielding Materials SBIR • Develop composites that provide more shielding per gram than Al • Tailor composition to enhance e or p shielding for specific mission • 20-30% improvement in shielding • thermal & mechanical properties • Sponsor: AFRL Materials RadFET • Commercial partner : Space Systems Loral • Phase 3 Flight Validation • Geosynchronous telecom satellite: Estrela Do Sul (2003-present) • 6 material samples, Al standards, 13 RadFET dosimeters Graph of Thickness/(Thickness)A* to (g/cm2)/g/cm2)A* Labels for Ge + W, GE = ZrHz, GE + Ni, GE + TiHz. 2000 x 500 km with 70Deg Incl. Slide 18 Radiation Shielding Composites The Goal: Replace Al, Ti and Be alloys with composite structures that: • Provide enhanced shielding to x-rays and neutrons. • Provide comparable strength for direct replacement in structural applications with no weight penalty. • Can be integrated into multifunctional structures. Neutron shielding Standard refractory PSI enriched B4C Advantages • Light weight/High strength • High temperature performance High volume fraction of absorbing materials • Composite architecture • Economical production process Neutron shielding graph with Standard refractory Axis Attenuation range 0 - 1.6 to Energy (eV) with range 10-5 to 10 to +7 Labels for PSI Model, Model Aluminum, Enr BrC Composite, Nat B4C Composite, Aluminum, Refract Composite Slide 19 Summary • PSI has several generations of charged particle instrumentation with flight pedigree • PSI’s radiation instrumentation may be able to support the human exploration requirements • Modular design and redundancy enable reconfiguration of LPD to serve multiple measurement requirements – energy range & particle types – G-factor & count rate – number of bins – Processing algorithms – multiple-axis • LPD test model (-TM) at PSI enables rapid and efficient breadboarding test and calibration of new configurations • PSI’s advanced shielding materials may be relevant for human exploration applications