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Published byAbel Wells Modified over 9 years ago
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Progress Towards Active Pixel Sensor Detectors for Solar Orbiter Dr Nick Waltham Head of Imaging Systems Division, Space Science & Technology Department, Rutherford Appleton Laboratory
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CCDs for Solar Physics... CCDs for Solar Physics e.g. SOHO, SMEI, SOLAR-B, STEREO... Future missions e.g. SDO But inherent limitations... External drive electronics needed. Solar physics community always want more pixels, more channels, faster readout. But with smaller/lower size, mass, and power ! And for Solar Orbiter... Radiation damage ! Protons, neutrons, etc Loss of charge transfer efficiency ! Pixel Size ? Smaller pixels yield a smaller instrument. STEREO CCD Solar Mass Ejection Imager (SMEI)
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RAL - Current programme... SMEI (Solar Mass Ejection Imager) CCD camera Birmingham University, UCSD, AFRL, Primary requirement - high dynamic range. Await launch STEREO/SECCHI solar science mission CCD camera design for 4 instruments with NRL and Birmingham. Key requirements - high speed readout, high dynamic range, yet reduced size, mass, and power. Now feeds into camera designs for SDO AO proposals. R&D Activities ASIC based CCD camera readout electronics. CMOS Active Pixel Sensors. Solar Mass Ejection Imager (SMEI) CCD ASICs Active Pixels
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What are we doing about it ? An alternative sensor technology to CCDs... Development of Science-grade CMOS Active Pixel Sensors !
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What is an Active Pixel Sensor (APS) ? Pixel Column Select Row Select Reset Photodiodes Reset Voltage Vdd Source Follower Image sensor with pixels. Wavelength coverage same as a CCD. Difference charge sensed inside pixel. Advantages... CMOS allows on-chip readout circuitry. Low mass, low power cameras. Smaller pixel size. S horter optics / smaller instrument. Charge sensed inside pixel... No charge transfer. Greater radiation tolerance. What are we doing about it... Science-Grade APS development Program.
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RAL APS Development Programme 1999 Design / modelling of pixel test structures (0.5 and 0.7 m CMOS). 2000 Fabrication and testing of pixel test structures. Established formal collaboration with Marconi (EEV) Exchange of designs / ideas, packaging, testing, Back-thinningUnique capability ! Design of 512 x 512 pixel sensor (0.5 m CMOS) 2001 Fabrication of 512 x 512 pixel prototype sensors. Birmingham join collaboration (Helen Mapson-Menard, Chris Eyles). EEV thinning test structures and 512 x 512 prototypes. First tests of 512 x 512 prototypes. Planning for Solar Orbiter (move to 0.25 m CMOS). 2002 Design / fabrication of 0.25 m CMOS 4kx3k 5 m pixel APS. Full testing of front and back-illuminated 512 x 512 prototypes.
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RAL APS test structure development Pixel DesignTest Structure chip with four 16 x 16 pixel arrays Test Results QE ~35% 10um active thickness Noise estimate < 50 electrons rms Calculated node capacitance = 18 fF Overall responsivity = 6 V per electron Peak output signal = 1 volt (167k electrons) Dark signal = 140 mV per second (0.6 nA/cm 2 ) Fixed pattern noise = 10mV pk-pk Quadradot Pixel Quantum Efficiency Helen Mapson-Menard Chris Eyles (Birmingham)
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512 x 512 Pixel Prototype Pixel Active Pixel Sensor 6 inch wafer of 512 x 512 sensors Wire-bonded to an evaluation PCB Individual 512 x 512 pixel APS chip
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512 x 512 Pixel Prototype Pixel Active Pixel Sensor Two test Images
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512 x 512 Pixel Prototype Pixel Active Pixel Sensor Note Dynamic range and Anti-blooming Performance ! So where next ?
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ESA’s Solar Orbiter Driven by the proposal of a Spectrometer on Solar Orbiter Detector Requirements EUV sensitive Large format (4k x 4k pixels) Small (5 m pixels) Science-grade linearity, low-noise, good uniformity Radiation hard Low power
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Solar Orbiter Detector Foveon's 16.8-million-pixel APS Detector Goals 4k x 4k pixel sensor 5 m pixel size 14 bit dynamic range EUV Sensitive 4-transistor CDS pixel 0.25 m rad-hard CMOS process Development Programme Refine requirement specification Develop CAD models and simulations Define architectural design Design, fabricate, and test 5 m pixel test structures Transfer 14-15 bit ADC to 0.25 m CMOS Investigate back-thinning with Marconi Demonstrate feasibility in time for the AO ! It can be done !
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Solar Orbiter Detector - Photodiode pixels. Standard APS pixel SO 4T pixel Column Output I bias Column Select Switch Reset Switch Source Follower Input MOS RST SEL Column Output I bias Transfer Gate RST SEL TX Simplest architecture. No kTC or Fixed-Pattern noise reduction. kTC and Fixed-Pattern noise reduction possible by differential readout of dark and signal level.
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Solar Orbiter Detector - Photodiode pixels. 4-MOS transistor pixel. PMOS transfer gate for kTC / FPN noise reduction and increased dynamic range. SchematicLayout
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Solar Orbiter Detector - Chip Architecture PIXEL SELECTION LOGIC 4K x 3K PIXEL ARRAY DIFFERENTIAL ANALOGUE OUTPUT DIFFERENTIAL AMPLIFIER A
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Solar Orbiter Detector - Progress 1.Area sensor: ESA’s Solar Orbiter for EUV imaging of Sun 4Kx3K, noise ~ 10 e- rms, DR ~ 12+ bits 2.Linear sensor: TOPSAT-2 BNSC Earth Observation 1 m ground resolution, colour, on-chip 10- bit ADCs, ~ 1500 fps 3.Electron sensor: HEP Vertex (Linear Collider, RHIC upgrade, biomed) intelligence in the pixel, fast readout (50MHz/row), low noise (~ 10 e- rms), data sparsification, radiation resistance 0.25 m CMOS manufactured by TSMC IC design / manufacturing sharing reduction of costs Linear sensor 4,000 pixels at 3 m pitch Electron sensor Area sensor 4,000 * 3,000 = 12 Million pixels 5 m pitch 1 2 3
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Solar Orbiter Detector - Progress 4k x 3k Sensor – Predictions from CAD simulation work Full Well Capacity ~ 46k electrons (5 m pixel) Readout Noise~ 10 electrons rms Dynamic Range~ 12+ bits Fill Factor~ 30% (but be careful !) Readout rate~ 1 MHz (through one port only) Readout time~ 12 seconds (full-frame, no windowing)
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Solar Orbiter Detector - Future Future Possibilities Chips of any format up to 4k x 4k (5 m) pixels. e.g. 4k x 512 (5 m) pixel strips on selected bands. 2k x 2k (10 m) pixels. or you could have odd-shaped pixels (10 x 20 m). CMOS allows you to design what you want ! Multi-port readout for higher frame rate. Windowed readout. Anything else wanted – besides EUV sensitivity ?
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EUV sensitivity – Backthinning, or FIB, or ? Two different approaches to enhance the EUV sensitivity of silicon APS. 1)Backthinning ( back- illumination): with Marconi Applied Technology 2)Front etching of the oxide by Focused Ion Beam
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Front vs Rear illumination Charge diffusion to adjacent pixels In field-free region EUV Photon < 5 m
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Solar Orbiter Detector - Future Development Programme 4k x 3k pixel Array Manufacture (Delivery Dec 02). Array Packaging (Jan 03). First light (Feb 03). Testing of 512 x 512 pixel prototypes (front and rear illuminated). E2V are delivering thinned sensors this week. Transfer of 14-15 bit ADC to 0.25 m CMOS in second phase. Thinning of 4k x 3k pixel array and EUV testing.
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Summary Requirement EUV Sensitivity 4k x 4k pixels 5 m pixel size Readout < 1 second Low power Cooling Radiation hardness Availability Science-grade CCD Yes Yes (for SDO ?) No Not easily No -80 °C Poor (CTE degradation) Soon (12 m pixels) ? (5 m pixels) APS Probably Yes Yes / Windowed readout Yes -80 °C Good (no CTE involved) (2003 – 2006) ?
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Solar Orbiter Detector - Alternatives Have considered naked CMOS APS so far. Are there alternatives ? Diamond / Bold ? Progress towards a large format array ? Smallest pixel ? / Bump bonding ? CID Radiation hard but limited availability, small range of formats, large pixels, very high read noise. Intensified APS – like in CDS ?
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