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Tracking Performances and Radiation Tolerance of Monolithic Active Pixel Sensors. G. Claus, C. Colledani, G. Deptuch, M.Deveaux, W. Dulinski, A.Gay, Yu. Gornushkin , A.Himmi, Ch. Hu-Guo, I.Valin, and M. Winter
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Tracking Performances and Radiation Tolerance of Monolithic Active Pixel Sensors. • G. Claus, C. Colledani, G. Deptuch, M.Deveaux, W. Dulinski, A.Gay, Yu. Gornushkin, A.Himmi, Ch. Hu-Guo, I.Valin,and M. Winter • IReS and LEPSI, IN2P3/ULP, 23, rue du Loess BP 23 (BP 20), F-67037 Strasbourg, France Outline: • Principle of operation of CMOS sensors • Resent results with first small prototypes (resolution, rad.tolerance) • Performances of 1st real scale prototype (3.5 cm2 , 1 million pixels) • Status of 1st prototype with column parallel readout and • integrated CDS • Summary
Idea and principle of operation • CMOS MAPS are replacing CCDs in visible light applications (still and video cameras, web-cameras, cell phones) – low power consumption, cheap! • To use them also for m.i.p. detection In Strasbourg (IReS-LEPSI) since 1999 • Twin-tub (double well) CMOS process with moderately doped epitaxial layer providing long minority carrier lifetime • Charge is generated in epitaxial layer (low doping): Q~80e--h/mm • Charge is collected through thermal diffusion by n-well/p-epi diode • No depletion potential applied • Potential barriers at layer interfaces confine the charge – improving collection efficiency • Charge-Voltage conversion on pixel • The device can be fabricated using a standard CMOS process, • P-type low resistivity Si g only NMOS transistors allowed
First Prototypes - Summary of Performances MIMOSA I die size 3.6 × 4.2 mm2 Examples of pixel layouts M I: 20× 20 µm2 Device internal architecture e.g. MIMOSA II High performances in m.i.p. detection established: S/N~30, e>99%, ssp~1.5-2 mm
Recent MIMOSA-1 results The spatial resolution as a function of ADC-bit encoding ( real signals “digitized” offline): even with 3-4 bits s ~2-3 mm Real particle clusters overlapped and combined distribution approximated by charge distribution function fot 2 hits. Hits are well separated at distances > 30 mm.
MIMOSA-4 test results: 0.35 mm AMS process without epitaxial layer but with low doping (resistivity) substrate • p-substrate process (~1015cm-3) • 4 arrays 64x64 pixels - pixel pitch 20x20 mm2 • diode (nwell/p-epi) size 2x2 mm2 - 1.8 fF • serial analogue readout - max. clock freq.: 20 MHz • die size 3.7x3.8 mm2 • technology 3M+2P • power supply 3.3 V • radiation tolerant transistor design • new structures of charge sensing elements: - charge spill-gate, - current mode pixel, - self-biasing diodes • Observed performances with 120 GeV/c p- at CERN-SPS: • Detection efficiency ~99.7% • S/N ~30 but charge spread is wider • Spatial resolution ~4 mm (20 mm pitch) Technology without epitaxial layer seems worth investigating and optimizing
Neutron radiation tolerance Chips irradiated with neutron sources at JINR and CEA-Saclay reactors were tested with Fe55 X-ray source. Noise as a function of fluence: Observed charge loss as a function of fluence: Charge loss is observed only for fluences >1011 n/cm2 what is 2 orders of magnitude more than it is expected for TESLA!
MIMOSA 5: big chip - simple quick start solution 19.4 mm One chip ~106 pixels of 17x17 mm2 • AMS 0.6 µm process with ~14 µm epitaxial layer • analogue readout - with hardware processing (CDS, pedestal subtraction, S/N analysis, sparsification on-line) • stitching: coarse - 100 µm + scribeline, option:precise – 1 mm • Lot of 6”wafers 44 kEuro 17.35 mm
MIMOSA-5 tests The chip (4 matrices of 512512 pixels (17x17 mm2 ) etched down to 120 mm was exposed to 120 GeV/c p- beam at CERN-SPS The same process as MIMOSA-1 the same performances expected? Noise larger than in case of MIMOSA-1 (different serial r.o.architecture – double source follower stage) Epitaxy layer ~14 mm charge ~1000e- Preliminary results: Noise mean ENC 20.7 e- Seed pixel S/N 23 Detection efficiency e~99.3%, ssp~1.7mm, sgain 2-3% close to those of MIMOSA-1
MIMOSA-5 response to inclined tracks(very preliminary): Total charge follows cos-1(q) S/N grows as well (saturation observed due to geometrical effect at large angles) MIMOSA-5 tests will continue in October 2002 at CERN-PS
MIMOSA-6 – first sensor with integrated signal processing • 0.35 MIETEC technology (same as MIMOSA-2) • IReS-LEPSI/DAPNIA collaboration • 24 column readout in parallel • 128 pixels per column • 5MHz effective readout frequency (30MHz clock, 6 clock cycles/pixel) • Amplification (x5.5),Correlated Double Sampling on pixel • Discriminators integrated on chip periphery (1 per column) • Power dissipation ~500 mW per column Chip layout: Pixel layout: 28x28 mm2 Matrix of 128x30 pixels AC coupling capacitor 29 transitstors Discriminators Chips are expected back from foundry this days. Test results - by the end of 2002. Charge storage capacitors
Summary: • The good performance of CMOS MAPS in charge particle detection has been succesfully established with 4 generations of small scale prototypes: • e99%, ssp~1.5-2.5 mm, S/N~30, s2hit~30 mm • Tolerance to neutrons exceeds TESLA requirements by more than 2 orders of magnitude! • Preliminary results from MIMOSA-5 tests indicate that these performances are reproducible with real size detectors • (~3.5 cm2, 120 mm thin) • First chip with integrated signal processing functions (CDS+A+D) is coming back from fabrication soon tests in October 2002 • R&D programme on CMOS MAPS TESLA Vertex Detector in a collaboration of 10 labs in F-UK-CH-NL-D+… is under way.