Monolithic Pixel Detector in a 0.15µm SOI Technology

Size: px
Start display at page:

Download "Monolithic Pixel Detector in a 0.15µm SOI Technology"

Transcription

1 Monolithic Pixel Detector in a 0.15µm SOI Technology 2006 IEEE Nuclear Science Symposium, San Diego, California, Nov. 1, 2006 Yasuo Arai (KEK) KEK Detector Technology Project : [SOIPIX Group] Y. Arai Y. Ikegami H. Ushiroda Y. Unno O. Tajima. Tsuboyama S. Terada M. Hazumi H. Ikeda A K. Hara B H. Ishino C T. Kawasaki D G. Varner E, E. Martin E, H. Tajima F, M. Ohno G, K. Fukuda G, H. Komatsubara G, J. Ida G, H.Hayashi G KEK JAXA A U. Tsukuba B TIT C Niigata U. D U. Hawaii E, SLAC F,OKI Elec. Ind. Co. G yasuo.arai@kek.jp (IEEE NSS) 1

2 Introduction Feature of SOI (Silicon-On-Insulator) Full Dielectric Isolation : Latchup Free, Small Area Low Junction Capacitance : High Speed, Low Power No Well junction, Thin Film : Low Leakage, Low Vth Shift (~300 ºC) Small Active Volume : High Soft Error Immunity yasuo.arai@kek.jp (IEEE NSS) 2

3 Feature of SOI Monolithic Pixel detector Bonded Wafer (High Resistive Substrate + Low Resistive Top Si). Standard CMOS Electronics (NMOS, PMOS, MIM Cap etc. can be used). Monolithic Detector, No Bump Bonds (Lower cost, Thin Device). High density (Smaller Pixel Size is possible). Small capacitance of the sense node (High gain V=Q/C) Industrial standard technology (Cost benefit and Scalability) Explore possibility of SOI detector for future experiments (ILC, SLHC, Super-Belle etc.) and other applications (Medical, Material etc.) yasuo.arai@kek.jp (IEEE NSS) 3

4 SOI Pixel Process Process SOI wafer Backside 0.15µm Fully-Depleted SOI CMOS process, 1 Poly, 5 Metal layers (OKI Electric Industry Co. Ltd.). Wafer Diameter: 150 mmφ, Top Si : Cz, ~18 Ω-cm, p-type, ~40 nm thick Buried Oxide: 200 nm thick Handle wafer: Cz >1k Ω-cm (No type assignment by supplier), 650 µm thick (SOITEC) Thinned to 350 µm, and plated with Al (200 nm). p+/n+ Implant and Contact formation yasuo.arai@kek.jp (IEEE NSS) 4

5 Diode TEG Metal contact & p+ implant Al (IEEE NSS) 5

6 p-n junction I-V characteristics n+ - back p+ - back Good Diode Characteristic Substrate is n type. ~700 Ω-cm (~6 x cm -3) yasuo.arai@kek.jp (IEEE NSS) 6

7 Pixel TEG CMOS Active Pixel Sensor Type 20 µm x 20 µm 32 x 32 pixels yasuo.arai@kek.jp (IEEE NSS) 7

8 Pixel Layout Window for Light Illumination (5.4 x 5.4 um 2 ) 6"φ MPW wafer 20 µm (pixel) 2.5 mm (chip) 2.5 mm (chip) p+ junction Storage Capacitance (100 ff) yasuo.arai@kek.jp (IEEE NSS) 8

9 Pixel I-V characterisitic V break ~ 100 V Hot Spot observed with infrared camera I = 40 µa, T = 1 min Corner of the bias ring Smooth the corner at next submission. (only 45 o allowed by design rule in previous run. next +30 o and 60 o ) yasuo.arai@kek.jp (IEEE NSS) 9

10 Laser Image Plastic Mask 32x32 image view with 670nm Laser and plastic mask Vdet = 10 V Laser (670 nm) Exposure Time = 7 µs yasuo.arai@kek.jp (IEEE NSS) 10

11 Response to β-ray source 90 Sr Performance test as a particle detector Output of one channel is observed with oscilloscope. Pixel sensor 90 Sr source yasuo.arai@kek.jp (IEEE NSS) 11

12 The voltage jump corresponds to a particle hit. V sense = Q C " 0.6 fc 8 ff = 70mV V det = 10 V W depletion ~ 44 µm Q ~ 3500 e (0.6 fc) Expected signal amplitude was observed for β-ray yasuo.arai@kek.jp (IEEE NSS) 12

13 Back Gate Effect Threshold Variation Back Gate IO Buffer Substrate Voltage act as Back Gate, and change transistor threshold. Signal disappears at 16V Consistent with SPICE simulation (IEEE NSS) 13

14 Back Bias Simulation and p+ location ENEXSS : 3D TCAD Simulator Back Gate effect can be reduced by placing p+ implant near transistors. D = (80, 5, 2 µm) NMOS BOX (200 nm) (5 µm wide p+, 1 x cm -3 ) Bulk: n- (~6 x cm -3 ) 350µm Backbias (0-100 V) Diode Electric Field yasuo.arai@kek.jp (IEEE NSS) 14

15 Summary We have started generic R&D on SOI detector. (Sensor in high-r Si and CMOS circuit in low-r Si). A first SOI Pixel Detector (32 x 32 pixels with 20µm x 20µm size) was successfully fabricated and tested. The detector is fabricated in a commercial 0.15 µm SOI CMOS process with 3 additional masks. Good images KEK06 with red laser light are taken. Signals of β-ray from 90 Sr are observed. Break down voltage of present sensor is about 100V and hot spot is identified. Back gate effect was obserbed. It is consistent with SPICE simulation, and studied with ENEXSS simulator. Next submission is scheduled in beginning of December yasuo.arai@kek.jp (IEEE NSS) 15

First Results of 0.15μm CMOS SOI Pixel Detector

First Results of 0.15μm CMOS SOI Pixel Detector First Results of 0.15μm CMOS SOI Pixel Detector International Symposium on Detector Development SLAC, CA, April 5, 2006 KEK Detector Technology Project : [SOIPIX Group] Yasuo Arai (KEK) Y. Arai Y. Ikegami

More information

First Results of 0.15µm CMOS SOI Pixel Detector

First Results of 0.15µm CMOS SOI Pixel Detector First Results of 0.15µm CMOS SOI Pixel Detector Y. Arai, M. Hazumi, Y. Ikegami, T. Kohriki, O. Tajima, S. Terada, T. Tsuboyama, Y. Unno, H. Ushiroda IPNS, High Energy Accelerator Reserach Organization

More information

Introduction to SoI pixel sensor. 27 Jan T. Tsuboyama (KEK) for KEK Detector R&D group Pixel Subgroup

Introduction to SoI pixel sensor. 27 Jan T. Tsuboyama (KEK) for KEK Detector R&D group Pixel Subgroup Introduction to SoI pixel sensor 27 Jan. 2006 T. Tsuboyama (KEK) for KEK Detector R&D group Pixel Subgroup Collaboration KEK Y. Unno, S. Terada, Y. Ikegami, T. Tsuboyama, M. Hazumi, O. Tajima, Y. Ushiroda,

More information

Tests of monolithic CMOS SOI pixel detector prototype INTPIX3 MOHAMMED IMRAN AHMED. Supervisors Dr. Henryk Palka (IFJ-PAN) Dr. Marek Idzik(AGH-UST)

Tests of monolithic CMOS SOI pixel detector prototype INTPIX3 MOHAMMED IMRAN AHMED. Supervisors Dr. Henryk Palka (IFJ-PAN) Dr. Marek Idzik(AGH-UST) Internal Note IFJ PAN Krakow (SOIPIX) Tests of monolithic CMOS SOI pixel detector prototype INTPIX3 by MOHAMMED IMRAN AHMED Supervisors Dr. Henryk Palka (IFJ-PAN) Dr. Marek Idzik(AGH-UST) Test and Measurement

More information

Progress on Silicon-on-Insulator Monolithic Pixel Process

Progress on Silicon-on-Insulator Monolithic Pixel Process Progress on Silicon-on-Insulator Monolithic Pixel Process Sep. 17, 2013 Vertex2013@Lake Starnberg Yasuo Arai, KEK yasuo.arai@kek.jp http://rd.kek.jp/project/soi/ 1 Outline Introduction Basic SOI Pixel

More information

Deep sub-micron FD-SOI for front-end application

Deep sub-micron FD-SOI for front-end application Nuclear Instruments and Methods in Physics Research A ] (]]]]) ]]] ]]] www.elsevier.com/locate/nima Deep sub-micron FD-SOI for front-end application H. Ikeda a,, Y. Arai b, K. Hara c, H. Hayakawa a, K.

More information

SOI Monolithic Pixel Detector Technology

SOI Monolithic Pixel Detector Technology Yasuo Arai 1, on behalf of the SOIPIX Collaboration High Energy Accelerator Research Organization (KEK) & The Okinawa Institute of Science and Technology (OIST) 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan

More information

Development of Integration-Type Silicon-On-Insulator Monolithic Pixel. Detectors by Using a Float Zone Silicon

Development of Integration-Type Silicon-On-Insulator Monolithic Pixel. Detectors by Using a Float Zone Silicon Development of Integration-Type Silicon-On-Insulator Monolithic Pixel Detectors by Using a Float Zone Silicon S. Mitsui a*, Y. Arai b, T. Miyoshi b, A. Takeda c a Venture Business Laboratory, Organization

More information

Measurement results of DIPIX pixel sensor developed in SOI technology

Measurement results of DIPIX pixel sensor developed in SOI technology Measurement results of DIPIX pixel sensor developed in SOI technology Mohammed Imran Ahmed a,b, Yasuo Arai c, Marek Idzik a, Piotr Kapusta b, Toshinobu Miyoshi c, Micha l Turala b a AGH University of Science

More information

A monolithic pixel sensor with fine space-time resolution based on silicon-on-insulator technology for the ILC vertex detector

A monolithic pixel sensor with fine space-time resolution based on silicon-on-insulator technology for the ILC vertex detector A monolithic pixel sensor with fine space-time resolution based on silicon-on-insulator technology for the ILC vertex detector, Miho Yamada, Toru Tsuboyama, Yasuo Arai, Ikuo Kurachi High Energy Accelerator

More information

Nuclear Instruments and Methods in Physics Research A

Nuclear Instruments and Methods in Physics Research A Nuclear Instruments and Methods in Physics Research A 636 (2011) S31 S36 Contents lists available at ScienceDirect Nuclear Instruments and Methods in Physics Research A journal homepage: www.elsevier.com/locate/nima

More information

Monolithic Pixel Sensors in SOI technology R&D activities at LBNL

Monolithic Pixel Sensors in SOI technology R&D activities at LBNL Monolithic Pixel Sensors in SOI technology R&D activities at LBNL Lawrence Berkeley National Laboratory M. Battaglia, L. Glesener (UC Berkeley & LBNL), D. Bisello, P. Giubilato (LBNL & INFN Padova), P.

More information

arxiv: v1 [physics.ins-det] 24 Jul 2015

arxiv: v1 [physics.ins-det] 24 Jul 2015 May 7, 2018 TID-Effect Compensation and Sensor-Circuit Cross-Talk Suppression in Double-SOI Devices arxiv:1507.07035v1 [physics.ins-det] 24 Jul 2015 Shunsuke Honda A, Kazuhiko Hara A, Daisuke Sekigawa

More information

MONOLITHIC pixel devices are an ultimate dream for

MONOLITHIC pixel devices are an ultimate dream for 2896 IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 56, NO. 5, OCTOBER 2009 Radiation Resistance of SOI Pixel Devices Fabricated With OKI 0.15 m FD-SOI Technology Kazuhiko Hara, Mami Kochiyama, Ai Mochizuki,

More information

SOFIST ver.2 for the ILC vertex detector

SOFIST ver.2 for the ILC vertex detector SOFIST ver.2 for the ILC vertex detector Proposal of SOI sensor for ILC: SOFIST SOI sensor for Fine measurement of Space and Time Miho Yamada (KEK) IHEP Mini Workshop at IHEP Beijing 2016/07/15 SOFIST ver.2

More information

arxiv: v2 [physics.ins-det] 14 Jul 2015

arxiv: v2 [physics.ins-det] 14 Jul 2015 April 11, 2018 Compensation of radiation damages for SOI pixel detector via tunneling arxiv:1507.02797v2 [physics.ins-det] 14 Jul 2015 Miho Yamada 1, Yasuo Arai and Ikuo Kurachi Institute of Particle and

More information

arxiv: v1 [physics.ins-det] 21 Jul 2015

arxiv: v1 [physics.ins-det] 21 Jul 2015 July 22, 2015 Compensation for TID Damage in SOI Pixel Devices arxiv:1507.05860v1 [physics.ins-det] 21 Jul 2015 Naoshi Tobita A, Shunsuke Honda A, Kazuhiko Hara A, Wataru Aoyagi A, Yasuo Arai B, Toshinobu

More information

Integrated diodes. The forward voltage drop only slightly depends on the forward current. ELEKTRONIKOS ĮTAISAI

Integrated diodes. The forward voltage drop only slightly depends on the forward current. ELEKTRONIKOS ĮTAISAI 1 Integrated diodes pn junctions of transistor structures can be used as integrated diodes. The choice of the junction is limited by the considerations of switching speed and breakdown voltage. The forward

More information

ILC VTX Issues being Addressed

ILC VTX Issues being Addressed ILC VTX Issues being Addressed Sensor Design Optimization studies for thin pixel device for Super-B upgrade Study of radiation hardness/max storage density High Performance/IR Design Experience with low

More information

Initial Characteristics and Radiation Damage Compensation of Double Silicon-on-Insulator Pixel Device

Initial Characteristics and Radiation Damage Compensation of Double Silicon-on-Insulator Pixel Device Initial Characteristics and Radiation Damage Compensation of Double Silicon-on-Insulator Pixel Device a, M. Asano a, S. Honda a, N. Tobita a, Y. Arai b, I. Kurachi b, S. Mitsui b, T. Miyoshi b, T. Tsuboyama

More information

Development of a monolithic pixel sensor based on SOI technology for the ILC vertex detector

Development of a monolithic pixel sensor based on SOI technology for the ILC vertex detector Accepted Manuscript Development of a monolithic pixel sensor based on SOI technology for the ILC vertex detector Shun Ono, Miho Yamada, Manabu Togawa, Yasuo Arai, Toru Tsuboyama, Ikuo Kurachi, Yoichi Ikegami,

More information

Simulation of High Resistivity (CMOS) Pixels

Simulation of High Resistivity (CMOS) Pixels Simulation of High Resistivity (CMOS) Pixels Stefan Lauxtermann, Kadri Vural Sensor Creations Inc. AIDA-2020 CMOS Simulation Workshop May 13 th 2016 OUTLINE 1. Definition of High Resistivity Pixel Also

More information

X-ray Radiation Hardness of Fully-Depleted SOI MOSFETs and Its Improvement

X-ray Radiation Hardness of Fully-Depleted SOI MOSFETs and Its Improvement June 4, 2015 X-ray Radiation Hardness of Fully-Depleted SOI MOSFETs and Its Improvement Ikuo Kurachi 1, Kazuo Kobayashi 2, Hiroki Kasai 3, Marie Mochizuki 4, Masao Okihara 4, Takaki Hatsui 2, Kazuhiko

More information

Session 3: Solid State Devices. Silicon on Insulator

Session 3: Solid State Devices. Silicon on Insulator Session 3: Solid State Devices Silicon on Insulator 1 Outline A B C D E F G H I J 2 Outline Ref: Taurand Ning 3 SOI Technology SOl materials: SIMOX, BESOl, and Smart Cut SIMOX : Synthesis by IMplanted

More information

Lecture #29. Moore s Law

Lecture #29. Moore s Law Lecture #29 ANNOUNCEMENTS HW#15 will be for extra credit Quiz #6 (Thursday 5/8) will include MOSFET C-V No late Projects will be accepted after Thursday 5/8 The last Coffee Hour will be held this Thursday

More information

PoS(Vertex 2011)043. SOI detector developments

PoS(Vertex 2011)043. SOI detector developments a, H. Katsurayama a,y. Ono a, H. Yamamoto a, Y. Arai b, Y. Fujita b, R. Ichimiya b, Y. Ikegami b, Y. Ikemoto b, T. Kohriki b, T. Miyoshi b, K. Tauchi b, S. Terada b, T. Tsuboyama b, Y. Unno b, T. Uchida

More information

Silicon Detectors in High Energy Physics

Silicon Detectors in High Energy Physics Thomas Bergauer (HEPHY Vienna) IPM Teheran 22 May 2011 Sunday: Schedule Semiconductor Basics (45 ) Silicon Detectors in Detector concepts: Pixels and Strips (45 ) Coffee Break Strip Detector Performance

More information

LSI ON GLASS SUBSTRATES

LSI ON GLASS SUBSTRATES LSI ON GLASS SUBSTRATES OUTLINE Introduction: Why System on Glass? MOSFET Technology Low-Temperature Poly-Si TFT Technology System-on-Glass Technology Issues Conclusion System on Glass CPU SRAM DRAM EEPROM

More information

Radiation Resistance ofsol Pixel Devices Fabricated with OKI O.151lID FD-SOI Technology

Radiation Resistance ofsol Pixel Devices Fabricated with OKI O.151lID FD-SOI Technology 2008 IEEE Nuclear Science Symposium Conference Record N04 5 Radiation Resistance ofsol Pixel Devices Fabricated with OKI O.151lID FD-SOI Technology K. Hara, M. Kochiyama, A. Mochizuki, T. Sega, Y. Arai,

More information

Electrical Characterization of a Second-gate in a Silicon-on-Insulator Transistor

Electrical Characterization of a Second-gate in a Silicon-on-Insulator Transistor Electrical Characterization of a Second-gate in a Silicon-on-Insulator Transistor Antonio Oblea: McNair Scholar Dr. Stephen Parke: Faculty Mentor Electrical Engineering As an independent double-gate, silicon-on-insulator

More information

Lecture: Integration of silicon photonics with electronics. Prepared by Jean-Marc FEDELI CEA-LETI

Lecture: Integration of silicon photonics with electronics. Prepared by Jean-Marc FEDELI CEA-LETI Lecture: Integration of silicon photonics with electronics Prepared by Jean-Marc FEDELI CEA-LETI Context The goal is to give optical functionalities to electronics integrated circuit (EIC) The objectives

More information

A flexible compact readout circuit for SPAD arrays ABSTRACT Keywords: 1. INTRODUCTION 2. THE SPAD 2.1 Operation 7780C - 55

A flexible compact readout circuit for SPAD arrays ABSTRACT Keywords: 1. INTRODUCTION 2. THE SPAD 2.1 Operation 7780C - 55 A flexible compact readout circuit for SPAD arrays Danial Chitnis * and Steve Collins Department of Engineering Science University of Oxford Oxford England OX13PJ ABSTRACT A compact readout circuit that

More information

IOLTS th IEEE International On-Line Testing Symposium

IOLTS th IEEE International On-Line Testing Symposium IOLTS 2018 24th IEEE International On-Line Testing Symposium Exp. comparison and analysis of the sensitivity to laser fault injection of CMOS FD-SOI and CMOS bulk technologies J.M. Dutertre 1, V. Beroulle

More information

MAPS-based ECAL Option for ILC

MAPS-based ECAL Option for ILC MAPS-based ECAL Option for ILC, Spain Konstantin Stefanov On behalf of J. Crooks, P. Dauncey, A.-M. Magnan, Y. Mikami, R. Turchetta, M. Tyndel, G. Villani, N. Watson, J. Wilson v Introduction v ECAL with

More information

CMOS Digital Integrated Circuits Lec 2 Fabrication of MOSFETs

CMOS Digital Integrated Circuits Lec 2 Fabrication of MOSFETs CMOS Digital Integrated Circuits Lec 2 Fabrication of MOSFETs 1 CMOS Digital Integrated Circuits 3 rd Edition Categories of Materials Materials can be categorized into three main groups regarding their

More information

Development of Pixel Detectors for the Inner Tracker Upgrade of the ATLAS Experiment

Development of Pixel Detectors for the Inner Tracker Upgrade of the ATLAS Experiment Development of Pixel Detectors for the Inner Tracker Upgrade of the ATLAS Experiment Natascha Savić L. Bergbreiter, J. Breuer, A. Macchiolo, R. Nisius, S. Terzo IMPRS, Munich # 29.5.215 Franz Dinkelacker

More information

Design and Performance of a Pinned Photodiode CMOS Image Sensor Using Reverse Substrate Bias

Design and Performance of a Pinned Photodiode CMOS Image Sensor Using Reverse Substrate Bias Design and Performance of a Pinned Photodiode CMOS Image Sensor Using Reverse Substrate Bias 13 September 2017 Konstantin Stefanov Contents Background Goals and objectives Overview of the work carried

More information

6. LDD Design Tradeoffs on Latch-Up and Degradation in SOI MOSFET

6. LDD Design Tradeoffs on Latch-Up and Degradation in SOI MOSFET 110 6. LDD Design Tradeoffs on Latch-Up and Degradation in SOI MOSFET An experimental study has been conducted on the design of fully depleted accumulation mode SOI (SIMOX) MOSFET with regard to hot carrier

More information

1 FUNDAMENTAL CONCEPTS What is Noise Coupling 1

1 FUNDAMENTAL CONCEPTS What is Noise Coupling 1 Contents 1 FUNDAMENTAL CONCEPTS 1 1.1 What is Noise Coupling 1 1.2 Resistance 3 1.2.1 Resistivity and Resistance 3 1.2.2 Wire Resistance 4 1.2.3 Sheet Resistance 5 1.2.4 Skin Effect 6 1.2.5 Resistance

More information

INTRODUCTION: Basic operating principle of a MOSFET:

INTRODUCTION: Basic operating principle of a MOSFET: INTRODUCTION: Along with the Junction Field Effect Transistor (JFET), there is another type of Field Effect Transistor available whose Gate input is electrically insulated from the main current carrying

More information

Recent Technological Developments on LGAD and ilgad Detectors for Tracking and Timing Applications

Recent Technological Developments on LGAD and ilgad Detectors for Tracking and Timing Applications Recent Technological Developments on LGAD and ilgad Detectors for Tracking and Timing Applications G. Pellegrini 1, M. Baselga 1, M. Carulla 1, V. Fadeyev 2, P. Fernández-Martínez 1, M. Fernández García

More information

problem grade total

problem grade total Fall 2005 6.012 Microelectronic Devices and Circuits Prof. J. A. del Alamo Name: Recitation: November 16, 2005 Quiz #2 problem grade 1 2 3 4 total General guidelines (please read carefully before starting):

More information

Wafer-scale 3D integration of silicon-on-insulator RF amplifiers

Wafer-scale 3D integration of silicon-on-insulator RF amplifiers Wafer-scale integration of silicon-on-insulator RF amplifiers The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation As Published

More information

Silicon on Insulator (SOI) Spring 2018 EE 532 Tao Chen

Silicon on Insulator (SOI) Spring 2018 EE 532 Tao Chen Silicon on Insulator (SOI) Spring 2018 EE 532 Tao Chen What is Silicon on Insulator (SOI)? SOI silicon on insulator, refers to placing a thin layer of silicon on top of an insulator such as SiO2. The devices

More information

Laser attacks on integrated circuits: from CMOS to FD-SOI

Laser attacks on integrated circuits: from CMOS to FD-SOI DTIS 2014 9 th International Conference on Design & Technology of Integrated Systems in Nanoscale Era Laser attacks on integrated circuits: from CMOS to FD-SOI J.-M. Dutertre 1, S. De Castro 1, A. Sarafianos

More information

http://clicdp.cern.ch Hybrid Pixel Detectors with Active-Edge Sensors for the CLIC Vertex Detector Simon Spannagel on behalf of the CLICdp Collaboration Experimental Conditions at CLIC CLIC beam structure

More information

Design Simulation and Analysis of NMOS Characteristics for Varying Oxide Thickness

Design Simulation and Analysis of NMOS Characteristics for Varying Oxide Thickness MIT International Journal of Electronics and Communication Engineering, Vol. 4, No. 2, August 2014, pp. 81 85 81 Design Simulation and Analysis of NMOS Characteristics for Varying Oxide Thickness Alpana

More information

INTRODUCTION TO MOS TECHNOLOGY

INTRODUCTION TO MOS TECHNOLOGY INTRODUCTION TO MOS TECHNOLOGY 1. The MOS transistor The most basic element in the design of a large scale integrated circuit is the transistor. For the processes we will discuss, the type of transistor

More information

Fabrication, Corner, Layout, Matching, & etc.

Fabrication, Corner, Layout, Matching, & etc. Advanced Analog Building Blocks Fabrication, Corner, Layout, Matching, & etc. Wei SHEN (KIP) 1 Fabrication Steps for MOS Wei SHEN, Universität Heidelberg 2 Fabrication Steps for MOS Wei SHEN, Universität

More information

The HGTD: A SOI Power Diode for Timing Detection Applications

The HGTD: A SOI Power Diode for Timing Detection Applications The HGTD: A SOI Power Diode for Timing Detection Applications Work done in the framework of RD50 Collaboration (CERN) M. Carulla, D. Flores, S. Hidalgo, D. Quirion, G. Pellegrini IMB-CNM (CSIC), Spain

More information

Semiconductor Memory: DRAM and SRAM. Department of Electrical and Computer Engineering, National University of Singapore

Semiconductor Memory: DRAM and SRAM. Department of Electrical and Computer Engineering, National University of Singapore Semiconductor Memory: DRAM and SRAM Outline Introduction Random Access Memory (RAM) DRAM SRAM Non-volatile memory UV EPROM EEPROM Flash memory SONOS memory QD memory Introduction Slow memories Magnetic

More information

Lecture 33 - The Short Metal-Oxide-Semiconductor Field-Effect Transistor (cont.) April 30, 2007

Lecture 33 - The Short Metal-Oxide-Semiconductor Field-Effect Transistor (cont.) April 30, 2007 6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007 Lecture 33-1 Lecture 33 - The Short Metal-Oxide-Semiconductor Field-Effect Transistor (cont.) April 30, 2007 Contents: 1. MOSFET scaling

More information

Lecture 020 ECE4430 Review II (1/5/04) Page 020-1

Lecture 020 ECE4430 Review II (1/5/04) Page 020-1 Lecture 020 ECE4430 Review II (1/5/04) Page 020-1 LECTURE 020 ECE 4430 REVIEW II (READING: GHLM - Chap. 2) Objective The objective of this presentation is: 1.) Identify the prerequisite material as taught

More information

Lecture 020 ECE4430 Review II (1/5/04) Page 020-1

Lecture 020 ECE4430 Review II (1/5/04) Page 020-1 Lecture 020 ECE4430 Review II (1/5/04) Page 020-1 LECTURE 020 ECE 4430 REVIEW II (READING: GHLM - Chap. 2) Objective The objective of this presentation is: 1.) Identify the prerequisite material as taught

More information

Fully depleted, thick, monolithic CMOS pixels with high quantum efficiency

Fully depleted, thick, monolithic CMOS pixels with high quantum efficiency Fully depleted, thick, monolithic CMOS pixels with high quantum efficiency Andrew Clarke a*, Konstantin Stefanov a, Nicholas Johnston a and Andrew Holland a a Centre for Electronic Imaging, The Open University,

More information

Active Pixel Sensors Fabricated in a Standard 0.18 um CMOS Technology

Active Pixel Sensors Fabricated in a Standard 0.18 um CMOS Technology Active Pixel Sensors Fabricated in a Standard.18 um CMOS Technology Hui Tian, Xinqiao Liu, SukHwan Lim, Stuart Kleinfelder, and Abbas El Gamal Information Systems Laboratory, Stanford University Stanford,

More information

Strip Detectors. Principal: Silicon strip detector. Ingrid--MariaGregor,SemiconductorsasParticleDetectors. metallization (Al) p +--strips

Strip Detectors. Principal: Silicon strip detector. Ingrid--MariaGregor,SemiconductorsasParticleDetectors. metallization (Al) p +--strips Strip Detectors First detector devices using the lithographic capabilities of microelectronics First Silicon detectors -- > strip detectors Can be found in all high energy physics experiments of the last

More information

Device Technologies. Yau - 1

Device Technologies. Yau - 1 Device Technologies Yau - 1 Objectives After studying the material in this chapter, you will be able to: 1. Identify differences between analog and digital devices and passive and active components. Explain

More information

New fabrication and packaging technologies for CMOS pixel sensors: closing gap between hybrid and monolithic

New fabrication and packaging technologies for CMOS pixel sensors: closing gap between hybrid and monolithic New fabrication and packaging technologies for CMOS pixel sensors: closing gap between hybrid and monolithic Outline Short history of MAPS development at IPHC Results from TowerJazz CIS test sensor Ultra-thin

More information

CMOS 0.18 m SPAD. TowerJazz February, 2018 Dr. Amos Fenigstein

CMOS 0.18 m SPAD. TowerJazz February, 2018 Dr. Amos Fenigstein CMOS 0.18 m SPAD TowerJazz February, 2018 Dr. Amos Fenigstein Outline CMOS SPAD motivation Two ended vs. Single Ended SPAD (bulk isolated) P+/N two ended SPAD and its optimization Application of P+/N two

More information

Design and characterisation of a capacitively coupled HV-CMOS sensor for the CLIC vertex detector

Design and characterisation of a capacitively coupled HV-CMOS sensor for the CLIC vertex detector CLICdp-Pub-217-1 12 June 217 Design and characterisation of a capacitively coupled HV-CMOS sensor for the CLIC vertex detector I. Kremastiotis 1), R. Ballabriga, M. Campbell, D. Dannheim, A. Fiergolski,

More information

Field-Effect Transistor (FET) is one of the two major transistors; FET derives its name from its working mechanism;

Field-Effect Transistor (FET) is one of the two major transistors; FET derives its name from its working mechanism; Chapter 3 Field-Effect Transistors (FETs) 3.1 Introduction Field-Effect Transistor (FET) is one of the two major transistors; FET derives its name from its working mechanism; The concept has been known

More information

UNIT III VLSI CIRCUIT DESIGN PROCESSES. In this chapter we will be studying how to get the schematic into stick diagrams or layouts.

UNIT III VLSI CIRCUIT DESIGN PROCESSES. In this chapter we will be studying how to get the schematic into stick diagrams or layouts. UNIT III VLSI CIRCUIT DESIGN PROCESSES In this chapter we will be studying how to get the schematic into stick diagrams or layouts. MOS circuits are formed on four basic layers: N-diffusion P-diffusion

More information

DEVICE AND TECHNOLOGY SIMULATION OF IGBT ON SOI STRUCTURE

DEVICE AND TECHNOLOGY SIMULATION OF IGBT ON SOI STRUCTURE Materials Physics and Mechanics 20 (2014) 111-117 Received: April 29, 2014 DEVICE AND TECHNOLOGY SIMULATION OF IGBT ON SOI STRUCTURE I. Lovshenko, V. Stempitsky *, Tran Tuan Trung Belarusian State University

More information

Radiation hardness improvement of FD-SOI MOSFETs for X-ray detector application

Radiation hardness improvement of FD-SOI MOSFETs for X-ray detector application Radiation hardness improvement of FD-SOI MOSFETs for X-ray detector application Ikuo Kurachi 1, Kazuo Kobayashi 2, Marie Mochizuki 3, Masao Okihara 3, Hiroki Kasai 4, Takaki Hatsui 2, Kazuo Hara 5, Toshinobu

More information

Metal-Oxide-Silicon (MOS) devices PMOS. n-type

Metal-Oxide-Silicon (MOS) devices PMOS. n-type Metal-Oxide-Silicon (MOS devices Principle of MOS Field Effect Transistor transistor operation Metal (poly gate on oxide between source and drain Source and drain implants of opposite type to substrate.

More information

EECS130 Integrated Circuit Devices

EECS130 Integrated Circuit Devices EECS130 Integrated Circuit Devices Professor Ali Javey 11/01/2007 MOSFETs Lecture 5 Announcements HW7 set is due now HW8 is assigned, but will not be collected/graded. MOSFET Technology Scaling Technology

More information

Fin-Shaped Field Effect Transistor (FinFET) Min Ku Kim 03/07/2018

Fin-Shaped Field Effect Transistor (FinFET) Min Ku Kim 03/07/2018 Fin-Shaped Field Effect Transistor (FinFET) Min Ku Kim 03/07/2018 ECE 658 Sp 2018 Semiconductor Materials and Device Characterizations OUTLINE Background FinFET Future Roadmap Keeping up w/ Moore s Law

More information

Diode Sensor Lab. Dr. Lynn Fuller

Diode Sensor Lab. Dr. Lynn Fuller ROCHESTER INSTITUTE OF TECHNOLOGY MICROELECTRONIC ENGINEERING Diode Sensor Lab Dr. Lynn Fuller Webpage: http://people.rit.edu/lffeee 82 Lomb Memorial Drive Rochester, NY 14623-5604 Tel (585) 475-2035 Fax

More information

on-chip Design for LAr Front-end Readout

on-chip Design for LAr Front-end Readout Silicon-on on-sapphire (SOS) Technology and the Link-on on-chip Design for LAr Front-end Readout Ping Gui, Jingbo Ye, Ryszard Stroynowski Department of Electrical Engineering Physics Department Southern

More information

Low Power Sensor Concepts

Low Power Sensor Concepts Low Power Sensor Concepts Konstantin Stefanov 11 February 2015 Introduction The Silicon Pixel Tracker (SPT): The main driver is low detector mass Low mass is enabled by low detector power Benefits the

More information

Simulation and test of 3D silicon radiation detectors

Simulation and test of 3D silicon radiation detectors Simulation and test of 3D silicon radiation detectors C.Fleta 1, D. Pennicard 1, R. Bates 1, C. Parkes 1, G. Pellegrini 2, M. Lozano 2, V. Wright 3, M. Boscardin 4, G.-F. Dalla Betta 4, C. Piemonte 4,

More information

Chapter 7 Introduction to 3D Integration Technology using TSV

Chapter 7 Introduction to 3D Integration Technology using TSV Chapter 7 Introduction to 3D Integration Technology using TSV Jin-Fu Li Department of Electrical Engineering National Central University Jungli, Taiwan Outline Why 3D Integration An Exemplary TSV Process

More information

Lecture 2. Part 2 (Semiconductor detectors =sensors + electronics) Segmented detectors with pn-junction. Strip/pixel detectors

Lecture 2. Part 2 (Semiconductor detectors =sensors + electronics) Segmented detectors with pn-junction. Strip/pixel detectors Lecture 2 Part 1 (Electronics) Signal formation Readout electronics Noise Part 2 (Semiconductor detectors =sensors + electronics) Segmented detectors with pn-junction Strip/pixel detectors Drift detectors

More information

Muon detection in security applications and monolithic active pixel sensors

Muon detection in security applications and monolithic active pixel sensors Muon detection in security applications and monolithic active pixel sensors Tracking in particle physics Gaseous detectors Silicon strips Silicon pixels Monolithic active pixel sensors Cosmic Muon tomography

More information

Development and Performance of. Kyoto s X-ray Astronomical SOI pixel sensor Sensor

Development and Performance of. Kyoto s X-ray Astronomical SOI pixel sensor Sensor Development and Performance of 1 Kyoto s X-ray Astronomical SOI pixel sensor Sensor T.G.Tsuru (tsuru@cr.scphys.kyoto-u.ac.jp) S.G. Ryu, S.Nakashima, Matsumura, T.Tanaka (Kyoto U.), A.Takeda, Y.Arai (KEK),

More information

Basic Fabrication Steps

Basic Fabrication Steps Basic Fabrication Steps and Layout Somayyeh Koohi Department of Computer Engineering Adapted with modifications from lecture notes prepared by author Outline Fabrication steps Transistor structures Transistor

More information

Contents 1 Introduction 2 MOS Fabrication Technology

Contents 1 Introduction 2 MOS Fabrication Technology Contents 1 Introduction... 1 1.1 Introduction... 1 1.2 Historical Background [1]... 2 1.3 Why Low Power? [2]... 7 1.4 Sources of Power Dissipations [3]... 9 1.4.1 Dynamic Power... 10 1.4.2 Static Power...

More information

Jan Bogaerts imec

Jan Bogaerts imec imec 2007 1 Radiometric Performance Enhancement of APS 3 rd Microelectronic Presentation Days, Estec, March 7-8, 2007 Outline Introduction Backside illuminated APS detector Approach CMOS APS (readout)

More information

Thin Silicon R&D for LC applications

Thin Silicon R&D for LC applications Thin Silicon R&D for LC applications D. Bortoletto Purdue University Status report Hybrid Pixel Detectors for LC Next Linear Collider:Physic requirements Vertexing 10 µ mgev σ r φ,z(ip ) 5µ m 3 / 2 p sin

More information

ECE520 VLSI Design. Lecture 2: Basic MOS Physics. Payman Zarkesh-Ha

ECE520 VLSI Design. Lecture 2: Basic MOS Physics. Payman Zarkesh-Ha ECE520 VLSI Design Lecture 2: Basic MOS Physics Payman Zarkesh-Ha Office: ECE Bldg. 230B Office hours: Wednesday 2:00-3:00PM or by appointment E-mail: pzarkesh@unm.edu Slide: 1 Review of Last Lecture Semiconductor

More information

PERSPECTIVES FOR DISRUPTIVE 200MM/8-INCH GAN POWER DEVICE AND GAN-IC TECHNOLOGY DR. DENIS MARCON SR. BUSINESS DEVELOPMENT MANAGER

PERSPECTIVES FOR DISRUPTIVE 200MM/8-INCH GAN POWER DEVICE AND GAN-IC TECHNOLOGY DR. DENIS MARCON SR. BUSINESS DEVELOPMENT MANAGER PERSPECTIVES FOR DISRUPTIVE 200MM/8-INCH GAN POWER DEVICE AND GAN-IC TECHNOLOGY DR. DENIS MARCON SR. BUSINESS DEVELOPMENT MANAGER What I will show you today 200mm/8-inch GaN-on-Si e-mode/normally-off technology

More information

Wafer-scale 3D integration of InGaAs image sensors with Si readout circuits

Wafer-scale 3D integration of InGaAs image sensors with Si readout circuits Wafer-scale 3D integration of InGaAs image sensors with Si readout circuits The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation

More information

CMOS Detectors Ingeniously Simple!

CMOS Detectors Ingeniously Simple! CMOS Detectors Ingeniously Simple! A.Schöning University Heidelberg B-Workshop Neckarzimmern 18.-20.2.2015 1 Detector System on Chip? 2 ATLAS Pixel Module 3 ATLAS Pixel Module MCC sensor FE-Chip FE-Chip

More information

EECS130 Integrated Circuit Devices

EECS130 Integrated Circuit Devices EECS130 Integrated Circuit Devices Professor Ali Javey 11/6/2007 MOSFETs Lecture 6 BJTs- Lecture 1 Reading Assignment: Chapter 10 More Scalable Device Structures Vertical Scaling is important. For example,

More information

Development of the Pixelated Photon Detector. Using Silicon on Insulator Technology. for TOF-PET

Development of the Pixelated Photon Detector. Using Silicon on Insulator Technology. for TOF-PET July 24, 2015 Development of the Pixelated Photon Detector Using Silicon on Insulator Technology for TOF-PET A.Koyama 1, K.Shimazoe 1, H.Takahashi 1, T. Orita 2, Y.Arai 3, I.Kurachi 3, T.Miyoshi 3, D.Nio

More information

MOSFET & IC Basics - GATE Problems (Part - I)

MOSFET & IC Basics - GATE Problems (Part - I) MOSFET & IC Basics - GATE Problems (Part - I) 1. Channel current is reduced on application of a more positive voltage to the GATE of the depletion mode n channel MOSFET. (True/False) [GATE 1994: 1 Mark]

More information

3-D Modelling of the Novel Nanoscale Screen-Grid Field Effect Transistor (SGFET)

3-D Modelling of the Novel Nanoscale Screen-Grid Field Effect Transistor (SGFET) 3-D Modelling of the Novel Nanoscale Screen-Grid Field Effect Transistor (SGFET) Pei W. Ding, Kristel Fobelets Department of Electrical Engineering, Imperial College London, U.K. J. E. Velazquez-Perez

More information

Transistor was first invented by William.B.Shockley, Walter Brattain and John Bardeen of Bell Labratories. In 1961, first IC was introduced.

Transistor was first invented by William.B.Shockley, Walter Brattain and John Bardeen of Bell Labratories. In 1961, first IC was introduced. Unit 1 Basic MOS Technology Transistor was first invented by William.B.Shockley, Walter Brattain and John Bardeen of Bell Labratories. In 1961, first IC was introduced. Levels of Integration:- i) SSI:-

More information

ECE 5745 Complex Digital ASIC Design Topic 2: CMOS Devices

ECE 5745 Complex Digital ASIC Design Topic 2: CMOS Devices ECE 5745 Complex Digital ASIC Design Topic 2: CMOS Devices Christopher Batten School of Electrical and Computer Engineering Cornell University http://www.csl.cornell.edu/courses/ece5950 Simple Transistor

More information

IMPROVED CURRENT MIRROR OUTPUT PERFORMANCE BY USING GRADED-CHANNEL SOI NMOSFETS

IMPROVED CURRENT MIRROR OUTPUT PERFORMANCE BY USING GRADED-CHANNEL SOI NMOSFETS IMPROVED CURRENT MIRROR OUTPUT PERFORMANCE BY USING GRADED-CHANNEL SOI NMOSFETS Marcelo Antonio Pavanello *, João Antonio Martino and Denis Flandre 1 Laboratório de Sistemas Integráveis Escola Politécnica

More information

Signal Integrity Design of TSV-Based 3D IC

Signal Integrity Design of TSV-Based 3D IC Signal Integrity Design of TSV-Based 3D IC October 24, 21 Joungho Kim at KAIST joungho@ee.kaist.ac.kr http://tera.kaist.ac.kr 1 Contents 1) Driving Forces of TSV based 3D IC 2) Signal Integrity Issues

More information

FUTURE PROSPECTS FOR CMOS ACTIVE PIXEL SENSORS

FUTURE PROSPECTS FOR CMOS ACTIVE PIXEL SENSORS FUTURE PROSPECTS FOR CMOS ACTIVE PIXEL SENSORS Dr. Eric R. Fossum Jet Propulsion Laboratory Dr. Philip H-S. Wong IBM Research 1995 IEEE Workshop on CCDs and Advanced Image Sensors April 21, 1995 CMOS APS

More information

J. E. Brau, N. B. Sinev, D. M. Strom University of Oregon, Eugene. C. Baltay, H. Neal, D. Rabinowitz Yale University, New Haven

J. E. Brau, N. B. Sinev, D. M. Strom University of Oregon, Eugene. C. Baltay, H. Neal, D. Rabinowitz Yale University, New Haven Chronopixe status J. E. Brau, N. B. Sinev, D. M. Strom University of Oregon, Eugene C. Baltay, H. Neal, D. Rabinowitz Yale University, New Haven EE work is contracted to Sarnoff Corporation 1 Outline of

More information

TECHNO INDIA BATANAGAR (DEPARTMENT OF ELECTRONICS & COMMUNICATION ENGINEERING) QUESTION BANK- 2018

TECHNO INDIA BATANAGAR (DEPARTMENT OF ELECTRONICS & COMMUNICATION ENGINEERING) QUESTION BANK- 2018 TECHNO INDIA BATANAGAR (DEPARTMENT OF ELECTRONICS & COMMUNICATION ENGINEERING) QUESTION BANK- 2018 Paper Setter Detail Name Designation Mobile No. E-mail ID Raina Modak Assistant Professor 6290025725 raina.modak@tib.edu.in

More information

PAPER SOLUTION_DECEMBER_2014_VLSI_DESIGN_ETRX_SEM_VII Prepared by Girish Gidaye

PAPER SOLUTION_DECEMBER_2014_VLSI_DESIGN_ETRX_SEM_VII Prepared by Girish Gidaye Q1a) The MOS System under External Bias Depending on the polarity and the magnitude of V G, three different operating regions can be observed for the MOS system: 1) Accumulation 2) Depletion 3) Inversion

More information

Semiconductor TCAD Tools

Semiconductor TCAD Tools Device Design Consideration for Nanoscale MOSFET Using Semiconductor TCAD Tools Teoh Chin Hong and Razali Ismail Department of Microelectronics and Computer Engineering, Universiti Teknologi Malaysia,

More information

Chapter 1. Introduction

Chapter 1. Introduction EECS3611 Analog Integrated Circuit esign Chapter 1 Introduction EECS3611 Analog Integrated Circuit esign Instructor: Prof. Ebrahim Ghafar-Zadeh, Prof. Peter Lian email: egz@cse.yorku.ca peterlian@cse.yorku.ca

More information

Design cycle for MEMS

Design cycle for MEMS Design cycle for MEMS Design cycle for ICs IC Process Selection nmos CMOS BiCMOS ECL for logic for I/O and driver circuit for critical high speed parts of the system The Real Estate of a Wafer MOS Transistor

More information

Wiring Parasitics. Contact Resistance Measurement and Rules

Wiring Parasitics. Contact Resistance Measurement and Rules Wiring Parasitics Contact Resistance Measurement and Rules Connections between metal layers and nonmetal layers are called contacts. Connections between metal layers are called vias. For non-critical design,

More information