Survey
* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Detectors and Analog Electronics Bill Crain The Aerospace Corporation 310-336-8530 [email protected] Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 1 28 September 2005 Introduction • • • • • • • • • Design Overview Requirements Flowdown Detector Specification Signals, Noise, and Processing Board Descriptions Interface Diagram Power Consumption Trade Studies Summary Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 2 28 September 2005 Detector Electronics Design Overview • Electronic Board Designs – Telescope Board – Analog Processing Board (APB) in E-box • Heritage approach from Polar CEPPAD/IPS unchanged from proposal – Linear pulse processing system with Amptek front-end – Circuits designed specifically for CRaTER requirements • Functional requirements summary – – – – Measure LET of high LET particles in thin detectors Measure LET of low LET particles in thick detectors Provide good resolution for TEP effects Robust to temperature drift and environments Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 3 28 September 2005 Functional Block Diagram Detector Boards Telescope Board Analog Processing Board Thin Thick Thin Thick Thin Thick Shaping Preamps Scaling Bias Networks Thermistor Baseline Restorer To Digital Board Timing Trigger Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 4 28 September 2005 Analog Signal Flow Diagram • Single fixed gain, linear transfer function • All detector channels use same topology Bias Network Silicon Detector Preamp dv/dt & Pole-Zero Cancellation Shaping Amp Analog Pulse Signals Scaling Amp Amp Test Pulser Timing Discrim. Digital Timing Signals Baseline Restorer Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 5 28 September 2005 Requirements Traceability Electronics Req. Thin Det. Thick Det. Parent Req. Affectivity Amplifier strings 3 3 CRaTER-L3-01 Board sizes Max. Energy Deposit 1 GeV 100 MeV CRaTER-L3-01 Preamp range, closedloop stability Low E Threshold Timing Threshold 2 MeV <1.3 MeV 200 keV <130 keV CRaTER-L3-01 Gain, baseline restorer, shaping time Noise (rms) < 400 keV < 40 keV CRaTER-L3-01 CRaTER-L2-08 Preamp, shaping time, thermal Max. Singles Rate 1.25 kHz 1.25 kHz CRaTER-L3-10 Shaping time, preamp time constant Integral non-linearity 0.1% 0.1% CRaTER-L2-08 Preamp, shaping amp Stability / drift 0.1% 0.1% CRaTER-L3-01 CRaTER-L2-08 Preamp, bias network, baseline restorer Internal Calibration 256:1 256:1 CRaTER-L3-08 Test pulser Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 6 28 September 2005 Detector Specification (1) • Document 32-05001 released rev 02 August 1, 2005 • Micron Semiconductor Limited – Lancing Sussex, UK • 20 years experience in supplying detectors for space physics – CEPPAD, CRRES, WIND, CLUSTER, ACE, IMAGE, STEREO, and more… • Detector Type – Ion-implanted doping to form P+ junction on N-type silicon – Very stable technology – Advantages to science include good carrier lifetime, stable to environmental conditions, and thin entrance windows Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 7 28 September 2005 Detector Specification (2) • Circular detectors having active area of 9.6 cm2 • Two different detector thicknesses: thin and thick – note: state-of-the-art is 20um for thin and 2,000um for thick detectors • Guard ring on P-side to improve surface uniformity • Very thin dead layers (windows) reduce energy loss, lower series resistance, and reduce noise E-field ~ 1mm Active Dimension (35mm) Gd/FP P+ Contact Grid P+ implant window Gd/FP Active Volume (depletion region) N window N contact 0.1 um Thickness 140 um thin; 1,000 um thick 0.1 um Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 8 28 September 2005 Detector Specification (3) • Detector drawings (Micron) – Note: this is not the present mount design Guard ring Al. contact plane Al. contact grid reduces surface resistivity Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 9 28 September 2005 Detector Design Requirements Summary Requirement Specification Active area 9.6 cm2 circular Active dimension 35 mm Active dimension tolerance +/- 0.1 mm Thickness Thin = 140 um, Thick = 1000 um Thickness tolerance +/- 10 um Thickness uniformity +/- 10 um Window 0.1 um ohmic, 0.1 um junction Metalization Ohmic surface and junction grid 3000 Å +/- 1000 Å Full depletion (FD) Thin = 20 – 40V, Thick = 150 – 200V Operating voltage max Thin = 2 x FD, Thick = FD + 30V Capacitance Thin = 700 pF, Thick = 100 pF Leakage current max (20C) Drift (max leakage @ 40C) Thin = 300 nA junction, 200 nA guard Thick = 1,000 nA junction, 700 nA guard 6 x Ileak @ 20C Stability 1% Ileak @ 40C for 168 hours Alpha resolution Thin = 45 KeV, Thick = 35 KeV FWHM Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 10 28 September 2005 Detector Specification (4) • ISO9001 – Full traceability and serialization – Travelers maintained • Qualification tests prior to flight detector shipment – – – – Bond pull test Random vibration test Thermal cycling Stability • Verification matrix specifies test criteria – – – – Leakage current Capacitance I-V characteristic Alpha resolution / pulser noise measurement Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 11 28 September 2005 Detector Verification Matrix Eye Chart From 32-05001 Rev 02 Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 12 28 September 2005 Proton Energy Deposition Simulations Thin 150MeV incident E 150 MeV Protons 10000 Nominal Threshold 20,000 incident protons Thin detectors (140 um) 100 10 0.1 Detector 1 Detector 3 Detector 6 20,000 incident protons Thick detectors (1000 um) 1000 Events Events 1000 1 0.01 Thick 150MeV incident E 150 MeV Protons 10000 Nominal Threshold GEANT4 100 10 1 10 1 0.01 100 10 100 Thick 1000MeV incident E 1 GeV Protons 10000 20,000 incident protons Thin detectors (140 um) 20,000 incident protons Thick detectors (1000 um) Detector 2 Detector 4 Detector 5 Detector 1 Detector 3 Detector 6 1000 1000 Events Events 1 Deposited Energy (MeV) Thin 1000MeV incident E 1 GeV Protons 100 10 1 0.01 Detector 2 Detector 4 Detector 5 0.1 Deposited Energy (MeV) 10000 Reference: M. Looper 100 10 0.1 1 10 Deposited Energy (MeV) 100 1 0.01 0.1 1 10 100 Deposited Energy (MeV) Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 13 28 September 2005 Iron Energy Deposition Simulation Reference: J.B. Blake Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 14 28 September 2005 Signal Characteristics Detector Min Signal Max Signal Collection Time Detector Capacitance Feedback Capacitance Thin 555E3 e-h pairs (88 fC) 275E6 e-h pairs (44 pC) 3 nsec e-drift 9 nsec h-drift 700 pF 15 pF Thick 55E3 e-h pairs (8.8 fC) 27.5E6 e-h pairs (4.4 pC) 38 nsec e-drift 115 nsec h-drift 100 pF 1.5 pF RFB CFB PreAmp Ao qμnNe(t)E qμpNh(t)E Cdet Vpk = Qtot/CFB CFB (Ao) >> Cdet Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 15 28 September 2005 Signal Processing (1) • Combined dynamic range of thin/thick pair is 5,000 • Thin threshold to provide overlap with thick range • Thin Detector Signal – Preamp input stage designed for 97% charge collection • High gain input jFET for large dynamic input capacitance • 4% drift in operating point will result in 0.1% in output peak – Large feedback capacitance needed to handle Fe deposit • Preamp compensation to maintain closed-loop stability • Thick Detector Signal – Not as sensitive to detector capacitance – Designed for low noise to maintain reliable 200 KeV low threshold and meet resolution requirement Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 16 28 September 2005 Noise Model (1) Detector Input Capacitance Leakage Current Shunt Resistance Series Resistance Preamp noise (ena) Thin 700 pF Det. 160 pF jFET+stray 200 nA @ 20C 800 nA @ 35C 6 Meg ohms 100 ohms 0.6 nV/√Hz Thick 100 pF Det 10 pF jFET+stray 1000 nA @ 20C 4000 nA @ 35C 6 Meg ohms 100 ohms 2.0 nV/√Hz + input cap. T=peaking time F=shaping factors Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 17 Reference: Helmuth Spieler IFCA Instrumentation Course Notes 2001 28 September 2005 Noise Model (2) Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 18 28 September 2005 Noise Model (3) 20C BOL Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 19 28 September 2005 Signal Processing (2) • Noise dominated by thick detector leakage current • Shaping time same for both thin and thick detectors – ~1 usec for comfortable PHA input timing – 3-pole gaussian shaping improves symmetry – 2-complex poles shortens tail • Coincidence Timing – Noise occupancy in 1-usec coincidence window < 0.1% – Threshold to noise ratio (T/N) ~ 3.2 for timing discriminator – Timing discriminator threshold ~ 130 keV • Anticipated BOL T/N ratio is ~ 10 • Allows margin for leakage current drift up to 10 uA Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 20 28 September 2005 Signal Processing (3) • Other factors affecting noise performance – Bias resistor on thin detector sized to minimize voltage drop – Bias resistor on thick detector sized to minimize noise – Detector shot noise doubles every 8 C • Beneficial to operate cold; preferably below 20 C Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 21 28 September 2005 Signal Processing (4) • Pileup is rare due to low event rate and relatively short shaping time – Exception: occasional periods of high ESP flux • Coincidence timing uncertainty from leading edge trigger is small – Amplified timing discriminator reduces time walk to acceptable 10% uncertainty • Ballistic deficit is not an issue due to short collection times relative to peaking time of shaper • Output voltage scaled for PHA input specifications Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 22 28 September 2005 Telescope Board Details Negative Bias Bias Network Test Pulser Test Input & Feedback Network Bias Network A250 JFET G P-contact Active Volume N-contact G Signal • Thin/thick detector pair use same design topology • Signal collected on P-contact • Guard signal shunted to ground • No guard leakage noise • AC coupling to isolate DC detector leakage current • Low noise / high gain JFET input stage (InterFET) with Amptek A250 hybrid • MIL-STD-5510 polyimide 8layer construction Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 23 28 September 2005 Analog Processing Board Details • Single board in E-box contains 3 thin and 3 thick detector processing channels – Polyimide laminate, MIL-STD-55110, 8-layers, 0.062 in. – Interfaces to digital board in same box • Components – Linear Technology radiation tolerant opamps for shaping stages, BLR, and comparators – Analog Devices rad tolerant op-amp for test pulser interface and bias monitoring (see trade study chart) • Pole-zero cancellation circuit included to prevent undershoot Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 24 28 September 2005 Analog Interface Block Diagram Aerospace MIT Analog Processing Digital Processing & Power +/- 6V, 5V & Returns Power Supply Detector Bias & Returns Shaped Pulse Analog Signals 3 thin, 3 thick Timing Digital Triggers 3 thin, 3 thick Pulse Height Analysis System Temperatures Spacecraft Interface • • • • ICD 32-02052 rev 01 +/- 6V power, 5V Thin and thick bias voltages Unipolar gaussian signals input to peak-hold circuits • Low-level triggers for coincidence timing • Test pulser level and clocking signals Test Pulser Trigger Test Pulser Level Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 25 28 September 2005 Power Estimate Detector Boards (total for 3 boards) Power Source Analog Processing Board Total Est. (mA) Total Max. (mA) 67.980 88.800 97.680 41.800 45.980 41.800 45.980 0.000 1.000 1.100 1.000 1.100 0.030 0.033 0.000 0.000 0.030 0.033 0.075 0.083 0.000 0.000 0.075 0.083 Power Est. (mW) 10% Uncertainty Power Est. (mW) 10% Uncertainty Total Est. (mW) Total Max. (mW) 187.5 206.25 626.6 689.26 814.1 895.51 Current Est. (mA) 10% Uncertainty Current Est. (mA) 10% Uncertainty 24-May-05 24-May-05 24-May-05 24-May-05 +6V Analog 27.000 29.700 61.800 -6V Analog 0.000 0.000 +5V Digital 0.000 -100V Thin Det Bias -300V Thick Det Bias Total Load Total estimated power dissipation is < 1 Watt Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 26 28 September 2005 Trade Studies • Considering detector bias current monitor – Housekeeping item to provide leakage current for each detector – No impact on noise or failure modes – Useful for diagnostic purposes especially during environmental testing of flight units Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 27 28 September 2005 Summary • Detectors are well-established technology from experienced supplier • Detector specification and Analog/Digital ICD documents have been released • Electronics design meets requirements of instrument requirements document 32-01205 Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 28 28 September 2005 Cosmic RAy Telescope for the Effects of Radiation Bill Crain, PDR Slide 29 28 September 2005