General status and plan Carried out extensive testing, obtained working pixels and promising radiation tolerance, just submitted engineering run 2013.

Slides:



Advertisements
Similar presentations
1 Annealing studies of Mimosa19 & radiation hardness studies of Mimosa26 Dennis Doering* 1, Samir Amar-Youcef 1,3,Michael Deveaux 1, Melissa Domachowski.
Advertisements

M. Szelezniak1PXL Sensor and RDO review – 06/23/2010 STAR PXL Sensors Overview.
Development of an Active Pixel Sensor Vertex Detector H. Matis, F. Bieser, G. Rai, F. Retiere, S. Wurzel, H. Wieman, E. Yamamato, LBNL S. Kleinfelder,
STATUS OF MEDIPIX-3, PLANS FOR TIMEPIX-2 X. Llopart.
Jaap Velthuis, University of Bristol SPiDeR SPiDeR (Silicon Pixel Detector Research) at EUDET Telescope Sensor overview with lab results –TPAC –FORTIS.
SOIPD Status e prospective for 2012 The SOImager2 is a monolithic pixel sensor produced by OKI in the 0.20 µm Fully Depleted- Silicon On Insulator (FD-SOI)
Snowmass 2005 SOI detector R&D Massimo Caccia, Antonio Bulgheroni Univ. dell’Insubria / INFN Milano (Italy) M. Jastrzab, M. Koziel, W. Kucewicz, H. Niemiec.
August SGSS front end, Summary August 2008 Edwin Spencer, SCIPP1 SGST Preview SCIPP, UC Santa Cruz Andrey Martchovsky Gregory Horn Edwin Spencer.
SPiDeR  First beam test results of the FORTIS sensor FORTIS 4T MAPS Deep PWell Testbeam results CHERWELL Summary J.J. Velthuis.
1 Improved Non-Ionizing Radiation Tolerance of CMOS Sensors Dennis Doering 1 *, Michael Deveaux 1, Melissa Domachowski 1, Michal Koziel 1, Christian Müntz.
Performance test of STS demonstrators Anton Lymanets 15 th CBM collaboration meeting, April 12 th, 2010.
First Results from Cherwell, a CMOS sensor for Particle Physics By James Mylroie-Smith
Pierpaolo Valerio.  CLICpix is a hybrid pixel detector to be used as the CLIC vertex detector  Main features: ◦ small pixel pitch (25 μm), ◦ Simultaneous.
1 Nick Sinev LCWS08, University of Illinois at Chicago November 18, 2008 Status of the Chronopixel project J. E. Brau, N. B. Sinev, D. M. Strom University.
2. Super KEKB Meeting, DEPFET Electronics DEPFET Readout and Control Electronics Ivan Peric, Peter Fischer, Christian Kreidl Heidelberg University.
07 October 2004 Hayet KEBBATI -1- Data Flow Reduction and Signal Sparsification in MAPS Hayet KEBBATI (GSI/IReS)
1 Digital Active Pixel Array (DAPA) for Vertex and Tracking Silicon Systems PROJECT G.Bashindzhagyan 1, N.Korotkova 1, R.Roeder 2, Chr.Schmidt 3, N.Sinev.
VI th INTERNATIONAL MEETING ON FRONT END ELECTRONICS, Perugia, Italy A. Dorokhov, IPHC, Strasbourg, France 1 NMOS-based high gain amplifier for MAPS Andrei.
1 Radiation damage effects in Monolithic Active Pixel Sensors Implemented in an 0.18µm CMOS process Dennis Doering, Goethe-University Frankfurt am Main.
Fully depleted MAPS: Pegasus and MIMOSA 33 Maciej Kachel, Wojciech Duliński PICSEL group, IPHC Strasbourg 1 For low energy X-ray applications.
Summary of CMS 3D pixel sensors R&D Enver Alagoz 1 On behalf of CMS 3D collaboration 1 Physics Department, Purdue University, West Lafayette, IN
Development of an ASIC for reading out CCDS at the vertex detector of the International Linear Collider Presenter: Peter Murray ASIC Design Group Science.
ALICE Inner Tracking System at present 2 2 layers of hybrid pixels (SPD) 2 layers of silicon drift detector (SDD) 2 layers of silicon strips (SSD) MAPs.
Specifications & motivation 2  Lowering integration time would significantly reduce background  Lowering power would significantly reduce material budget.
LEPSI ir e s MIMOSA 13 Minimum Ionising particle Metal Oxyde Semi-conductor Active pixel sensor GSI Meeting, Darmstadt Sébastien HEINI 10/03/2005.
CEA DSM Irfu 20 th october 2008 EuDet Annual Meeting Marie GELIN on behalf of IRFU – Saclay and IPHC - Strasbourg Zero Suppressed Digital Chip sensor for.
Recent developments on Monolithic Active Pixel Sensors (MAPS) for charged particle tracking. Outline The MAPS sensor (reminder) MIMOSA-22, a fast MAPS-sensor.
8 July 1999A. Peisert, N. Zamiatin1 Silicon Detectors Status Anna Peisert, Cern Nikolai Zamiatin, JINR Plan Design R&D results Specifications Status of.
J. Crooks STFC Rutherford Appleton Laboratory
PHASE-1B ACTIVITIES L. Demaria – INFN Torino. Introduction  The inner layer of the Phase 1 Pixel detector is exposed to very high level of irradiation.
AMS HVCMOS status Raimon Casanova Mohr 14/05/2015.
Valerio Re, Massimo Manghisoni Università di Bergamo and INFN, Pavia, Italy Jim Hoff, Abderrezak Mekkaoui, Raymond Yarema Fermi National Accelerator Laboratory.
Technology Overview or Challenges of Future High Energy Particle Detection Tomasz Hemperek
65 nm CMOS analog front-end for pixel detectors at the HL-LHC
A. Rivetti Villa Olmo, 7/10/2009 Lepix: monolithic detectors for particle tracking in standard very deep submicron CMOS technologies. A. RIVETTI I.N.F.N.
ClicPix ideas and a first specification draft P. Valerio.
Thanushan Kugathasan, CERN Plans on ALPIDE development 02/12/2014, CERN.
26 Apr 2009Paul Dauncey1 Digital ECAL: Lecture 2 Paul Dauncey Imperial College London.
BTeV Hybrid Pixels David Christian Fermilab July 10, 2006.
10th Trento Workshop on Radiation Detectors HVCMOS Sensors for LHC Upgrade Felix Michael Ehrler, Robert Eber Daniel Münstermann, Branislav Ristic, Mathieu.
Irfu saclay Development of fast and high precision CMOS pixel sensors for an ILC vertex detector Christine Hu-Guo (IPHC) on behalf of IPHC (Strasbourg)
System IC Design Lab. Dongguk University 1 Study of CERN for the ALICE ITS upgrade Study of CERN for the ALICE ITS upgrade KIM,D.H., KWON,Y.,SONG,M.K.
Sensor testing and validation plans for Phase-1 and Ultimate IPHC_HFT 06/15/ LG1.
CMOS MAPS with pixel level sparsification and time stamping capabilities for applications at the ILC Gianluca Traversi 1,2
Improvement of ULTIMATE IPHC-LBNL September 2011 meeting, Strasbourg Outline  Summary of Ultimate test status  Improvement weak points in design.
TIMELINE FOR PRODUCTION 2  Need to be ready for production end next year  => submission of final mask set ~September 2015  Would like one more iteration.
BeamCal Electronics Status FCAL Collaboration Meeting LAL-Orsay, October 5 th, 2007 Gunther Haller, Dietrich Freytag, Martin Breidenbach and Angel Abusleme.
A. Dorokhov, IPHC, Strasbourg, France 1 Description of pixel designs in Mimosa22 Andrei Dorokhov Institut Pluridisciplinaire Hubert Curien (IPHC) Strasbourg,
CMOS Sensors WP1-3 PPRP meeting 29 Oct 2008, Armagh.
-1-CERN (11/24/2010)P. Valerio Noise performances of MAPS and Hybrid Detector technology Pierpaolo Valerio.
Eleuterio SpiritiILC Vertex Workshop, April On pixel sparsification architecture in 130nm STM technology ILC Vertex Workshop April 2008 Villa.
MISTRAL & ASTRAL: Two CMOS Pixel Sensor Architectures dedicated to the Inner Tracking System of the ALICE Experiment R&D strategy with two main streams.
Trends in MONOLITHIC DETECTORS and ADVANCED CMOS MANUFACTURING W. Snoeys ESE Seminar October 14 th 2014 PH-ESE-ME,
RD53 1.  Full/large demonstrator chip submission ◦ When: 2016 A.Early 2016: If chip must have been fully demonstrated in test beams for TDRs to be made.
Technical status of the Gossipo-3 : starting point for the design of the Timepix-2 March 10, Vladimir Gromov NIKHEF, Amsterdam, the Netherlands.
Ideas on MAPS design for ATLAS ITk. HV-MAPS challenges Fast signal Good signal over noise ratio (S/N). Radiation tolerance (various fluences) Resolution.
Hybrid CMOS strip detectors J. Dopke for the ATLAS strip CMOS group UK community meeting on CMOS sensors for particle tracking , Cosenors House,
Irfu saclay CMOS Pixel Sensor Development: A Fast Readout Architecture with Integrated Zero Suppression Christine HU-GUO on behalf of the IRFU and IPHC.
Pixel Sensors for the Mu3e Detector Dirk Wiedner on behalf of Mu3e February Dirk Wiedner PSI 2/15.
Clear Performance and Demonstration of a novel Clear Concept for DEPFET Active Pixel Sensors Stefan Rummel Max-Planck-Institut für Physik – Halbleiterlabor.
1 /28 LePIX – Front End Electronic conference – Bergamo 25 May 2011 – Piero Giubilato LePIX – monolithic detectors in advanced CMOS Collection electrode.
Charge sensitive amplifier
Results achieved so far to improve the RPC rate capability
Digital readout architecture for Velopix
LHCC Upgrade Session, 12 March 2013
HV-MAPS Designs and Results I
Rita De Masi IPHC-Strasbourg on behalf of the IPHC-IRFU collaboration
HVCMOS Detectors – Overview
OmegaPix 3D IC prototype for the ATLAS upgrade SLHC pixel project 3D Meeting 19th March, 2010 A. Lounis, C. de La Taille, N. Seguin-Moreau, G.
Stefano Zucca, Lodovico Ratti
Presentation transcript:

General status and plan Carried out extensive testing, obtained working pixels and promising radiation tolerance, just submitted engineering run 2013 : optimize pixel structure and study different options for the readout architecture to obtain medium/large scale demonstrator 2014 : finalize full scale to be ready for volume production 2 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

PIXEL REQUIREMENTS 3  W/cm2 power budget is upper limit  Lowering power would significantly reduce material budget ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

 Analog:  Determined by collected charge over capacitance (Q/C) in the pixel => pixel sensor optimization  Digital:  Determined by on-chip architecture & cluster size  Architecture:  Rolling shutter: pursued by RAL and by IPHC  Other architectures with in-pixel binary front-end (CERN):  Priority encoder  Orthopix (several projections in addition to X and Y)  Data transmission off-chip:  Determined by cluster size unless data reduction by clustering algorithm Power consumption: 3 components 4 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

6

MIMOSA32 chips 7  Characterization measurements with:  55 Fe source (double peak at ~1640 electrons)  Testbeam: 6 GeV π - in T10 from PS  Note: Signal from MIP in 18 micron thick epitaxial layer 80*18=1440 electrons  Extracted values:  Noise in electrons  Signal to Noise Ratio (SNR)  Cluster size  Charge Collection Efficiency (CCE) ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

MIMOSA32 chips: Results 55 Fe measurements P7: Dnwell (sq. ~20 μm2), 3T_ll, ELT P2: Nwell_1 (octo, ~10.9 μm2), 3T_ll, ELT P7 V ADC = 1350 mV P2 V ADC = 1350 mV Chip Structur e Noise (e - )CCE seedCCE clusterCluster Size Mean cluster size 9B P721,451,299,352,9 P219,146,497,153,5 8 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

MIMOSA32 chips: Variation of V diode 9 V diode up to 1.3 V: Shift of the spectrum towards higher ADC values V diode larger than 1.4 V: No big differences observed Results from Strasbourg confirmed Example: - Chip: 9B - Structure: P00 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

 Results on first prototype designed by IPHC Strasbourg promising, significant variation as a function of diode bias  Submitted another prototype to study and optimize pixel  Contains two 1.8x1.8mm matrices of 20x20 and 30x30 micron pixels with different geometries for the collection electrode and surroundings  First measurements see below Prototype July 2012 submission: Explorer0 10 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Floorplan July submission revisited Pixel matrix 90x90 20x20um pixels Analog : current mirrors/buffer/pulsing Digital circuit to control readout Pads 1. 2x2 octogonal 2. 3x3 octogonal 3. 4x4 octogonal 4. 3x3 square 5. 3x3 octo midspace 6. 3x3 octo maxspace 7. 2x2 octo max+space tw 8. 3x3 octogonal tw 9. 3x3 octo maxspace tw Green: pulsed rows (2 per submatrix) Pixel matrix 60x60 30x30um pixels ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

More detail on the collection electrodes 12 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Fe-55 spectrum 13 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Fe-55 spectrum 14 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Fe-55 spectrum 15 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Fe-55 spectrum 16 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Fe-55 spectrum 17 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Fe-55 spectrum 18 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Fe-55 spectrum 19 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Fe-55 spectrum 20 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Extracted capacitance (assuming the collection of 1640 electrons) < 5 fF 21 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Cluster sizes 22 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Cluster sizes 23 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Cluster sizes 24 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Cluster sizes 25 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Cluster sizes 26 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Cluster sizes 27 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Cluster sizes 28 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Cluster sizes 29 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Testbeam setup 30 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Landaus 31 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Efficiency & fake hit rate (explorer chip) 32 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013  High efficiency at low fake hit rates  Reverse substrate bias gives extra margin

 Observed:  Fully functional pixels  MPV increase and cluster size decrease with increasing back bias  Cluster size increase with decreasing collection electrode size  MPV is not affected by pixel size, but increases at low biases with decreasing collection electrode size and increasing spacing  Very high efficiencies with very low hit rates  Capacitance contribution from routing: 2.1fF, full circuit with routing = 4.6 fF  Less than 5 fF total at -8 V for some pixels => detector capacitance less than 1 fF  Can reduce circuit contribution to reach ~1-2 fF total  Done for engineering run which is now being submitted Explorer chip (July 2012 submission) 33 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Further pixel sensor improvement 34  For the July 2012 submission we obtain ~50mV per hit but distributed over several pixels, and optimization should give at least a factor of 2  Could we reach “digital signal” (250mV) on a single pixel and save more power? Several options:  Thicker epi/high resistivity substrate will increase signal  Lower doping/higher resistivity for more depletion (in combination with reverse substrate bias) and lower cluster size/multiplicity  Further lowering input capacitance  … ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

IN PIXEL HIT DISCRIMINATION 36 VRESET  Large gain amplifier/comparator discharges ~ 80fF storage capacitor when the sensor receives a particle hit  Storage capacitor instead of full flip-flop to save space  Allows other readout architectures AMPL/CO MP ENABLE RESET ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Front-End and Memory layout 37 Block Size: 10.5 x 22.0 µm 2 Memory size: 6.9 x 7.3 µm 2 Custom shape NMOS cap with L > 10 um Circuitry in deep pwell (except the collection electrode) ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Output signal example Qin (electrons) Time walk ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Minimum detectable charge 39 Minimum detectable charge definition Minimum detectable charge as a function of the bias current Cd = 1 fF Ith = 0.5 nA Ileak = 5 pA Noise at threshold 14e (nominal 20nA condition) Memory state (V) Qin (electrons) ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

 RAL & Strasbourg:  Rolling shutter architecture  Strasbourg also in-pixel discriminator/ADC  CERN :  Digital architectures requiring low power front end with discriminator in the pixel  Priority encoder:  Multiple projections (orthopix)Architecture 41 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Priority Encoder readout 42  Data driven readout of the pixel matrix, only zero-suppressed data are transferred to the periphery.  Asynchronous circuit with no clock propagation into the pixel matrix:  Power reduction.  Noise reduction (no clock disturbance in to the analog part). End of Column logic Pixels arranged in columns Layout view digital analog separate address bus per column Each clock cycle the memory of the pixel with the highest priority is reset and its address is sent to the periphery. ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Priority Encoder – Pixel layout µm + 10 µm 22 µm Collection electrode Part of Priority Encoder Analog Front End Memory cell Analog Front End Memory cell Collection electrode Priority encoder reset state ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

IMPLEMENTATION IN ENGINEERING RUN 44  Mxt_CERN1...4  In total  4 variants of priority encoder matrix  16 explorer matrices  Several test structures PRIORITY ENCODER EXPLORER TEST ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

ORTHOPIX 45  Based on multiple projections to reduce ambiguities  Already four well chosen projections X, Y, U and V yield good reconstruction results for outer layers  Allows data (and power) reduction : for four projections data reduced from N^2 pixels to 4N signals  2 255x255 pixel matrices + one smaller matrix implemented in engineering run  NOTE: LVDS driver/receiver ORTHOPIX LVDS TEST ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

SEUCHIP 46  Contains array of single port, dual port memory and shift register  Allows Single Event Upset testing ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

March 2013 engineering run 48  CERN/INFN/WUHAN: explorer, priority encoder and orthopix matrix in several variants and test structures  Two variants of LVDS driver  RAL: three matrices with rolling shutter  IPHC: many matrices with rolling shutter, also significant work on zero suppression circuitry.  Several starting materials: P. Riedler  Engineering run will require very significant test program => will need to plan ahead ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Total Ionizing Dose test on transistors 50 X-Ray tube ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Example: low voltage NMOS transistor 51 I 0 = 100 nA. W/L TID (Mrad) W/L = 0.22 um / 0.18 um -> I 0 = nA  Curves do not change significantly with irradiation  Extensive testing campaign on transistors now almost complete and radiation tolerance in excess of ALICE needs ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

RADIATION TOLERANCE (1Mrad n/cm 2 ) 52 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013  Signal not changed, noise increased as expected  Neutron and proton irradiated explorer samples give promising results, analysis in progress

DESIGN TOWARDS FULL CHIP/SYSTEM 54  Would like to submit simplified large scale chip in July, important for system aspects  Need to design/debug/optimize several circuit blocks (see next slide) and would like to submit a more complex large scale chip towards the end of the year ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

DESIGN TOWARDS FULL CHIP/SYSTEM 1) Pixel sensor optimization: CERN/WUHAN 2) Pixel matrix: CERN/WUHAN 3) Digital readout circuitry in the periphery: INFN 4) Serializer/LVDS driver: INFN 5) Power regulation: some interest from NIKHEF 6) On-chip pulser for self-test 7) Configuration and Monitoring 1) SEU tolerant registers + I/O 2) DAC for bias 3) ADC for monitoring 4) Monitoring: Temperature, Power consumption, Detector leakage, chip ID STILL SIGNIFICANT MANPOWER NEEDED, especially in 5-7 but also in ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

TESTING 56  This year we will receive many different pixels  different starting materials  different anode geometries  Different frontends  Different readout architectures  We need to characterise them for  Noise behavior (low noise setup)  Charge collection efficiency (radioactive sources)  Position dependent efficiency (laser light)  Detection efficiency (test beam)  Radiation hardness (all tests above after irradiation)  Distribution of work (and electrical test systems) amongst institutes is extremely important  Perhaps we will already have the first module assemblies ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

COMMON TEST SYSTEM DEVELOPMENT 57 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

COMMON TEST SYSTEM DEVELOPMENT 58 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

TESTING 59 MIMOSA32 MIMOSA34 Explorer-0 Explorer-1 CHERWEL L2 CERN digital readout SEU NoiseN/A Fe-55N/A Test beam LaserN/A All before and after irradiation (neutrons, X-ray) ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

CONCLUSIONS 60  Pixel sensor  50mV distributed over a few pixels, with prospect of at least 2x improvement  Could we get to digital signal by further optimization?  Analog front end design: 40nW* pixels = 10 mW/cm 2  Digital: looking at solution around 10mW/cm 2  Off-chip data transmission ~ 30-50mW/chip or <10mW/cm 2 Trying to approach strip level power consumption per unit area and definitely stay below 100mW/cm 2  Radiation tolerance sufficient for Alice  Significant work in design and in test participation needed ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

61 THANK YOU ! ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Transient Noise 62 t = 200 ns : hit t = 50 us : sample and reset Analog Output Memory State Memory state samples histogram Repeated every 50 us ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Noise - Error Function Fit 63 Qin (electrons) Memory on state 1 rate µ = electrons σ = 13.8 electrons Ibias = 20 nA Cd = 1 fF ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Noise vs. detector capacitance 64 thr 1 fF20 nA500 pA5 pA105 e - 14 e fF20 nA500 pA5 pA260 e - 27 e fF50 nA250 nA5 pA133 e - 20 e fF50 nA250 nA1 nA129 e - 18 e ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

MOS transistor matching 65 Extracted value from simulation NMOS: A Vth = 3.43 mV µm PMOS:A Vth = 3.25 mV µm Monte Carlo simulation in ADE XL environment for mismatch statistical variation. Process statistical variation seems to be not available. ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

Noise vs. detector capacitance 66 µ = electrons σ = 3.0 electrons Memory on state 1 rate Ibias = 20 nA Cd = 1 fF ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013

RADIATION TOLERANCE (ionizing 3 Mrad) 67 ALICE ITS UPGRADE MEETING – Seoul, April 5-6, 2013