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CMOS Sensors WP1-3 PPRP meeting 29 Oct 2008, Armagh CMOS Technology • CMOS = Complimentary Metal Oxide Semiconductor – Efficient way to build electronics out of NMOS and PMOS transistors • Technology appeared in 70’s – Driven by consumer electronics market – Used in PP for electronics/computing • PP Holy Grail: integrated sensor and readout electronics • Difference in requirements – Industry: digital; visible light imaging – PP: analogue and digital at the same time; detection of ionizing particles MAPS: Monolithic Active Pixel Sensors • Signal detected in thin epi-layer, < 20 mm – Localized, excellent precision 1 mm – Small signal, collection by diffusion • Low noise – Small capacitance • Amplification in pixel allows to preserve good Signal-to-Noise • Limited choice as only NMOS transistors are allowed – PMOS transistors compete for charge • Several PP groups follow the approach of using existing processes – MIMOSA sensors, …. Future Trends • Affordable thin, low power and precise sensors will revolutionize Particle Physics • World-wide interest but only few groups have design capability and access to this technology – Fermilab, KEK, Strasbourg, INFN, LBL, RAL – Expensive with complicated IP management • Trend is to put more functionality inside pixels – Started to be addressed in the last years (ex. deep nwell MAPS by INFN, vertical wafer integration by Fermilab) • UK is leading in two directions – INMAPS: allows full CMOS inside pixel – ISIS: allows raw charge storage INMAPS • Standard MAPS does not allow CMOS – Parasitic collection of charge by other n-wells • Shield n-wells with deep p+ implant – Ion beam of MeV energy which stops at certain depth • Full CMOS capability – Increased complexity – Reduced power consumption • RAL/CALICE pioneered this process for PP – Huge potential, a lot of interest from outside of PP ISIS: In Situ Storage • Another way to enhance CMOS functionality • Storage of raw charge – Excellent noise immunity – Reduced power consumption • Implemented as n+ buried channel (as in CCD) and deep p+ implant • Pioneered by LCFI for PP – Only group with access to this technology 4T Structures • 4T (four transistors) structures allows efficient charge capture and amplification – Now standard process offered by foundries – Offers better noise immunity – Need studies for small signal transfers from larger capacitor SPIDER Programme • Based on three processes, INMAPS, ISIS and 4T which are unique in PP • Buried channel (ISIS) – Have prove of concept: ISIS1 – Produced buried channel in CMOS technology: ISIS2 • Deep p+ (INMAPS) – TPAC: first device to use INMAPS – Cherwell: distributed architecture • 4T process – For Cherwell: first attempt to use 4T for scientific application • Several years ahead of other groups – Deep p+ planned by other groups but no practical implementation so far – Strong interest in INMAPS multi-project runs ISIS3 • ISIS2 produced by LCFI in 2008 – Test bed device with many variants – Used to optimize ISIS3 • ISIS3 – Refining the process – Putting in more functionality – Reducing pixel size (currently 10x80 mm2 ) Current load 80 μm 10 μm Source follower Pad ISIS2 Pixel Geometry TPAC2 • Large scale sensor – Uses INMAPS – Architecture inspired by TPAC1 chip • Designed for system applications – DCAL tests TPAC1 Cherwell (CDS circuit) COL • Distributed functionality with no dead areas CS CR BIAS + ∑ VTH TRIM – Enabled by INMAPS – Rolling shutter readout MEMORY [0] Control logic MEMORY [1] MEMORY [2] MEMORY [3] MEMORY [4] MEMORY [5] MEMORY [6] – Better noise immunity COL COL • Cherwell will explore 4T architecture for particle detection for the first time COL WrEn MEMORY [7] RESET 1x SRAM SELECT Pixel Boundary 50 um pixel boundary 4 T 4 T 4 T WP1: Sensor Design • Design team based at RAL Sensor Specification Preliminary Design Review • Design Specification • Design reviews – Oversees progress – External Experts • Submissions • Handling of IP issues Intermediate Design Review Final Design Review Sign-Off Chip Submission WP2: Sensor Modelling • Signal collection – ISIS: charge collection through opening in deep p+ – TPAC/Cherwell: collection efficiency • Signal transfer – 4T: transfer of small signal from a large capacitance load – ISIS: charge transfer in buried channel Charge collection in TPAC Charge collection in ISIS WP3: Sensor Characterization • Share facilities and expertise between institutions Signal/Noise measurements (Oxford,Imperial, Bristol) Source Tests Initial tests (RAL) (RAL) Sensor Evaluation Laser Tests Test Beams (RAL) (Bristol) Irradiation Cosmics (Bristol) (Birmingham) WP3: Sensor Characterization • Signal and Noise – Radioactive sources 55Fe, 90Sr – Performance integrated over pixels TPAC1 55Fe signal • Laser and source mapping – 1064 and 660 nm lasers – Strong source to exercise individual pixels – Charge collection – Threshold trimming (TPAC) ISIS1 Laser Map Irradiation and Test Beams • Irradiations will determine sensor longevity in experiments – Surface damage – Bulk damage – Necessary to validate new processes for wider applications MAPS before/after irradiation • Two test beams, in 2010 and 2011 – Essential to measure coordinate resolution and efficiency ISIS1 test beam Knowledge Exchange • Several pixel technologies were driven by PP • CMOS technology was not driven by Particle Physics but this may change – INMAPS and ISIS modifications to standard CMOS introduce very attractive features for other applications – STFC and UK have leading positions • ISIS: fast X-ray imaging – Fast framing CCD imagers based on ISIS principle are commercially produced • Deep p+ (INMAPS) can be used for any fast and specialized industrial imaging Sensor Summary • Pixel sensors with complex integrated functionality is the future • SPIDER will address this by R&D in three directions: ISIS, INMAPS and 4T • Sensor programme is based on – ISIS3, TPAC, Cherwell – Integrated approach to design, modelling and testing • Looking for applications outside of PP