999999-1 XYZ 10/2/2016 MIT Lincoln Laboratory APS-2 Status Vyshi Suntharalingam, Tony Soares, Rich D’Onofrio May 30, 2008.

Slides:



Advertisements
Similar presentations
Radiation damage in silicon sensors
Advertisements

Derek Wright Monday, March 7th, 2005
P. Fernández-Martínez – Optimized LGAD Periphery25 th RD50 Workshop, CERN Nov Centro Nacional de MicroelectrónicaInstituto de Microelectrónica.
1 CCD RAIN (PHOTONS) BUCKETS (PIXELS) VERTICAL CONVEYOR BELTS (CCD COLUMNS) HORIZONTAL CONVEYOR BELT ( SERIAL REGISTER ) MEASURING CYLINDER (OUTPUT AMPLIFIER)
MIT Lincoln Laboratory 3-D Kickoff 1 CLK 4/7/00 3D Circuit Integration Technology for Multiproject Fabrication 7 April, 2000 James Burns, Andy Curtis,
Solid State Detectors-2
Simulation of the Electrostatic potential and the Electric Field in Pixel device By Joseph Manungu High Energy Physics Group meeting Dept of Physics Syracuse.
Sample Devices for NAIL Thermal Imaging and Nanowire Projects Design and Fabrication Mead Mišić Selim Ünlü.
Ronald Lipton Hiroshima D Sensors - Vertical Integration of Detectors and Electronics Contents: Introduction to three dimensional integration of.
20th RD50 Workshop (Bari)1 G. PellegriniInstituto de Microelectrónica de Barcelona G. Pellegrini, C. Fleta, M. Lozano, D. Quirion, Ivan Vila, F. Muñoz.
CMOS and Microfluidic Hybrid System on Chip for Molecule Detection Bowei Zhang, Qiuchen Yuan, Zhenyu Li, Mona E. Zaghloul, IEEE Fellow Dept. of Electrical.
Bulk Silicon CCDs, Point Spread Functions, and Photon Transfer Curves: CCD Testing Activities at ESO Mark Downing, Dietrich Baade, Sebastian Deiries, (ESO/Instrumentation.
MIT Lincoln Laboratory XYZ 9/15/2015 APS-2 Chip: W21 R5C6 Has Quartz Support.
Development of a new microfluidic analysis system on silicon with different nanostructures as sensitive elements Mihaela Miu, Irina Kleps, Florea Craciunoiu,
Dahee Kim (Ewha womans university) for MPC-EX collaboration TEST OF MINI-PAD SILICON SENSOR FOR PHENIX MPC-EX.
Waveguide High-Speed Circuits and Systems Laboratory B.M.Yu High-Speed Circuits and Systems Laboratory 1.
Silicon – On - Insulator (SOI). SOI is a very attractive technology for large volume integrated circuit production and is particularly good for low –
Medipix sensors included in MP wafers 2 To achieve good spatial resolution through efficient charge collection: Produced by Micron Semiconductor on n-in-p.
1 Marco Ferrero With Nicolo’ Cartiglia, Francesca Cenna, Fabio Ravera, Universita’ degli Studi di Torino & INFN.
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.
Prospect for Si sensors in Korea Y. Kwon (Yonsei Univ.)
Effect of Metal Overhang on Electric Field for Pixel Sensors Kavita Lalwani, Geetika Jain, Ranjeet Dalal, Kirti Ranjan & Ashutosh Bhardwaj Department of.
Lecture 24a, Slide 1EECS40, Fall 2004Prof. White Lecture #24a OUTLINE Device isolation methods Electrical contacts to Si Mask layout conventions Process.
INTEGRATED CIRCUITS Dr. Esam Yosry Lec. #3. Diffusion  Introduction  Diffusion Process  Diffusion Mechanisms  Why Diffusion?  Diffusion Technology.
Foundry Characteristics
Silicon detector processing and technology: Part II
16 sept G.-F. Dalla BettaSCIPP Maurizio Boscardin a, Claudio Piemonte a, Alberto Pozza a, Sabina Ronchin a, Nicola Zorzi a, Gian-Franco Dalla Betta.
MIT Lincoln Laboratory NU Status-1 JAB 11/20/2015 Advanced Photodiode Development 7 April, 2000 James A. Burns ll.mit.edu.
1 FNAL Pixel R&D Status R. Lipton Brief overview due to 3 failed MS Powerpoint versions –3D electronics New technologies for vertical integration of electronics.
Budapest University of Technology and Economics Department of Electron Devices Solution of the 1 st mid-term test 20 October 2009.
CERN, November 2005 Claudio Piemonte RD50 workshop Claudio Piemonte a, Maurizio Boscardin a, Alberto Pozza a, Sabina Ronchin a, Nicola Zorzi a, Gian-Franco.
Update on Simulation and Sensor procurement for CLICPix prototypes Mathieu Benoit.
Budapest University of Technology and Economics Department of Electron Devices Microelectronics, BSc course Operation of PN junctions:
Technology Overview or Challenges of Future High Energy Particle Detection Tomasz Hemperek
XYZ 1/7/2016 MIT Lincoln Laboratory APS-2 Diode Simulation First Look V. Suntharalingam 27 July 2007.
-1-CERN (11/24/2010)P. Valerio Noise performances of MAPS and Hybrid Detector technology Pierpaolo Valerio.
P. Fernández-Martínez – Optimized LGAD PeripheryRESMDD14, Firenze 8-10 October Centro Nacional de MicroelectrónicaInstituto de Microelectrónica de.
Infrared Laser Test System Silicon Diode Testing 29 May 2007 Fadmar Osmić Contents: Setup modifications new amplifier (Agilent MSA-0886) new pulse generator.
Latest news on 3D detectors IRST CNM IceMos. CNM 2 wafers fabricated Double side processing with holes not all the way through, (aka Irst) n-type bulk.
Realizing 3D Smart Dust Particles Zeynep Dilli. 11 April 2005 Introduction & Outline MIT Lincoln Laboratories FDSOI Process: Adapted to chip stacking.
Development of SOI pixel sensor 28 Sep., 2006 Hirokazu Ishino (Tokyo Institute of Technology) for SOIPIX group.
Pixel Meeting Nov 7, Status Update on Sensors and 3D Introduction Laser Annealed HPK sensors MIT-LL thinned sensors SOI devices –OKI –ASI 3D assembly.
Low Mass, Radiation Hard Vertex Detectors R. Lipton, Fermilab Future experiments will require pixelated vertex detectors with radiation hardness superior.
TCT measurements of HV-CMOS test structures irradiated with neutrons I. Mandić 1, G. Kramberger 1, V. Cindro 1, A. Gorišek 1, B. Hiti 1, M. Mikuž 1,2,
3D Simulation Studies of Irradiated BNL One-Sided Dual-column 3D Silicon Detector up to 1x1016 neq/cm2 Zheng Li1 and Tanja Palviainen2 1Brookhaven National.
Development of N-in-P Silicon Strip and Pixel sensors for very high radiation environments Y. Unno For the Collaboration of KEK, Univ. Tsukuba and Hamamatsu.
Testsystems PXD6 - testing plans overview - by Jelena NINKOVIC Hybrid Boards for PXD6 - by Christian KOFFMANE Source measurements on DEPFET matrices using.
Infineon CoolIR2DieTM Power Module
Fully Depleted Low Power CMOS Detectors
New Mask and vendor for 3D detectors
Daniela Bortoletto, Amitava Roy, Carsten Rott, Gino Bolla
Characterization and modelling of signal dynamics in 3D-DDTC detectors
Charge collection studies with irradiated CMOS detectors
EMT362: Microelectronic Fabrication
Status of 3D detector fabrications at CNM
Fully depleted CMOS sensor using reverse substrate bias
Bonding interface characterization devices
V. Suntharalingam 5 February 2008
Fab. Example: Piezoelectric Force Sensor (1)
TCAD Simulation of Geometry Variation under HPK campaign
Thin Planar Sensors for Future High-Luminosity-LHC Upgrades
HR CHESS News Jens (et. al.).
Hexagons and 8” Sensor R&D Ron Lipton
SCIENTIFIC CMOS PIXELS
Silicon pixel detectors and electronics for hybrid photon detectors
Semiconductor Detectors
New UK-Planar Pixel mask
Effects of LER on MOSFET Electrical Behavior
New detectors are needed! Prototype Characterization
Fabrication of 3D detectors with columnar electrodes of the same doping type Sabina Ronchina, Maurizio Boscardina, Claudio Piemontea, Alberto Pozzaa, Nicola.
Presentation transcript:

XYZ 10/2/2016 MIT Lincoln Laboratory APS-2 Status Vyshi Suntharalingam, Tony Soares, Rich D’Onofrio May 30, 2008

MIT Lincoln Laboratory XYZ 10/2/2016 Status Items Diode capacitance and leakage extraction Plan for SOI FET noise testing New test board for 3D APS-2 imager chip testing (Tony) –We will send a pdf of schematic separately Overview of MIT-LL APS-2 testing hardware and software (Rich) Deliver packaged Back Illuminated imagers (no quartz) –MB21B wafer 9 R5C6 –MB21B wafer 9 R4C3 –MB21A wafer 3 R2C3 –None of these were tested at MIT-LL

MIT Lincoln Laboratory XYZ 10/2/2016 Pixel Capacitance and Leakage Extraction Back Illuminated APS2 Imager New measurements with Keithley 4200-SCS (better software and hardware control) Imager tested after Back Illumination (thinned to 50µm) and pad sputter –Test Area=4160 pixels * (24  m) 2 –Substrate: n-type 3000 ohm-cm ~1.5e12 cm -3 Full depletion not detectable –Dominated by lateral capacitance to Channel Stops –At 10V: 11.5fF/pixel, 70fA/pixel Scupper Pixels (p+) (VSCP) 4 pixels wide Substrate Contact (n+) Ring (VPDBIAS) 4 pixels wide 256 x 256 pixel array (p+ side of each diode connected to Tier-2 SOI circuit) C-meter Current(pA/pix)

MIT Lincoln Laboratory XYZ 10/2/2016 Insight from Simulation (7/27/07) Pixel #3 (p+) n-CS n-3000 ohm-cm (3e12 /cm3) 50 um Depth n-substrate contact 5 x 24 um Width Doping Profiles

MIT Lincoln Laboratory XYZ 10/2/2016 Two-Dimensional Simulation of 5 Pixels Potential Contours Show Effect of Varying Substrate Bias Vsub=0V Vsub=2VVsub=5V Vsub=10V Vsub=14V 0V 2V 5V 10V Vsub=14V Potential (V) Potential profile at center of pixel-3 (vertical “cut-line”) Depth into Si “cut-line” (filename error) For Vsub=10V, 15V: E-field is vertical from ~25 to 50 um depth into silicon. Nearer to the frontside we observe the lateral influence of the Channel Stops From 7/27/07

MIT Lincoln Laboratory XYZ 10/2/2016 Reverse Bias of 15V Vsub=15V (at backside) 15V 0V 8.5 um 18 Microns 0V From 7/27/07 C lateral C substrate