Control of the fabrication process for the sensors of the CMS Silicon Strip Tracker. Anna Macchiolo. CMS Collaboration

Size: px
Start display at page:

Download "Control of the fabrication process for the sensors of the CMS Silicon Strip Tracker. Anna Macchiolo. CMS Collaboration"

Transcription

1 Control of the fabrication process for the sensors of the CMS Silicon Strip Tracker Anna Macchiolo Universita di Firenze- INFN Firenze on behalf of the CMS Collaboration 6 th International Conference on Large Scale Applications and Radiation Hardness of Semiconductor Detectors

2 Sensor Fabrication Center HPK Silicon Sensor Test Strategy in CMS Control & Distribution Center CERN & Production Committee Sensor Fabrication Center STM The aim of the Process Qualification Centers Florence Strasbourg Vienna is to ensure a constant quality throughout the production and to monitor the companies process 25% 25% 25% 25% Quality Test Center Pisa Quality Test Center Perugia Quality Test Center Vienna Quality Test Center Karlsruhe The CMS SST is in full sensor production phase: 35 % of HPK sensors 15 % of STM sensors have been already delivered 1% sensors ~5% ts Irradiation Qualification Centers Louvain, Karlsruhe ~5% ts Bonding Test Centers Pisa, Strasbourg >5% ts Process Qualification & Stability Centers Florence Strasbourg, Vienna More than 1200 test-structures have been tested by the PQC Centers up to now (during the pre-production we have largely exceeded the nominal assignment of 5 % of the total number of t.s.) RD03 Process Quality Control for the CMS SST Anna Macchiolo 2

3 SST Standard test-structures Standard Half Moon A common set of 9 test structures with the same design is inserted in all the SST wafers, whatever the sensor type (rectangular or wedge) or the producer is. The test-structures allows to perform measurements that are not possible on the main sensor or destructive tests. RD03 Process Quality Control for the CMS SST Anna Macchiolo 3

4 The Standard Half-Moon 26 AC coupled strips: quality of the integrated capacitor dielectric Gate Controlled Diode : surface current at the Si- SiO 2 interface IV on minisensor from 0 to 700 V CV on diode Bulk resistivity Sheet: 9 superficial structures to monitor Aluminum and p+ surface resistivity, poly-silicon resistors value 9 AC coupled strips: inter-strip capacitance 9 DC coupled strips: interstrip resistance CV on MOS Flat Band Voltage RD03 Process Quality Control for the CMS SST Anna Macchiolo 4

5 PQC Set-Up The PQC equipment in the Florence clean-room RD03 Process Quality Control for the CMS SST Anna Macchiolo 5

6 PQC Hardware GPIB 40 channels Probestation Switching box 4 multiplexers multiplexers 10 x 1 10 A Source Measure Unit Probe-card Switching matrix 4 x 5 C Vsource LCR It has been possible to adopt the same set-up in the three PQC centers because the labs have common or very similar equipment. During the pre-production phase a calibration program among the three labs has been followed with an exchange of test-structures to ensure the full compatibility of results. Computer running Labview RD03 Process Quality Control for the CMS SST Anna Macchiolo 6

7 Acquisition Software The Labview acquisition program: performs the 9 measurements in an automatic run analyses and fit the results when necessary set a flag that identifies the positive outcome of the test. Results are stored: The results of the measurements are visualized in the Labview front-panel to allow an easy check of the output. in local files in a XML file that can be inserted directly in the centralized database for the CMS Tracker construction in Lyon. A complete test takes about 30 minutes RD03 Process Quality Control for the CMS SST Anna Macchiolo 7

8 The PQC measurements and first results RD03 Process Quality Control for the CMS SST Anna Macchiolo 8

9 Quality of the dielectric in the integrated capacitors Test on an array of 26 AC coupled strips Both in HPK and STM the capacitor dielectric is composed by thin layers of SiO 2 and Si 3 N 4 Constance in time of the capacitance value (Cac > 1.2 pf/cm per µm of implanted strip) Breakdown voltage of the dielectric layer of the capacitor (defined as the voltage at which the current across the dielectric is > 10 µa) It is foreseen that during catastrophic beam-loss events (expected at the level of 1-2 per year) a voltage difference around one hundred Volts can be present at the two faces of the capacitors Structures/ bin Structures/ bin Breakdown voltage of the dielectric layer HPK Our acceptance criteria is V break > 120 V STM Voltage applied to the dielectric The measurement is performed between 0 and 200 V Voltage applied to the dielectric RD03 Process Quality Control for the CMS SST Anna Macchiolo 9

10 Quality of the inter-strip insulator In the Standard Moon the MOS and GCD are built with the thicker oxide (1 2 µm) that characterizes the inter-strip region in the full-size sensor Measurement of the Flat Band Voltage at 100 KHz with the CV on MOS (V fb < 10 V) Measurement of Surface Current with the IV on a square GCD (I GCD < 100 pa) Total Capacitance (F) 1.4E E E E E E-10 Accumulation Fitted value of Vfb = 1.2 V Diode current (A) 8.0E E E E E E E E-11 Fitted value of the surface current = 40 pa Accumulation 2.3E-10 Inversion 4.0E-11 Inversion 3.0E E E-11 -Gate Voltage (V) Gate Voltage (V) RD03 Process Quality Control for the CMS SST Anna Macchiolo 10

11 Problem with the Vfb in STM Flat Band Voltage vs Production Time (STM) Switching from the R&D to the production line in STM at the beginning of 2003 caused some problems. We have found several batches with high Vfb. This effect has been traced back to the contamination introduced by a particular machine that has been now excluded from the production line. Flat Band Voltage (V) A single episode in week # 10 of 2002 Contaminated batches at the beginning of 2003 allowed Vfb range Year x week of production RD03 Process Quality Control for the CMS SST Anna Macchiolo 11

12 Dependence of the inter-strip capacitance on the Vfb value Irradiating the test-structures at fluences equivalent to 10 years of LHC has shown that a high Vfb, connected to a bad quality of the inter-strip Si oxide, leads to a large increase in the inter-strip capacitance. 1,2 1,1 Interstrip Capacitance [pf] 1,2 1,1 1,0 0,9 0,8 0,7 Before Irradiation: V FB =5V V FB =7V V FB =20V V FB =38V 0, Strip Number Interstrip Capacitance [pf] 1,0 0,9 0,8 0,7 After Irradiation: V FB =5V V FB =7V V FB =20V V FB =38V Proton irradiation at the cyclotron of the Forschungszentrum Karlsruhe 0, Strip Number RD03 Process Quality Control for the CMS SST Anna Macchiolo 12

13 Diode Depletion Voltage (V) Bulk resistivity The CMS Tracker request to have depletion voltages below 400 V after 10 LHC years leads to the following requirements on the bulk resistivity measured with CV at 100 KHz on diode: 1.25 < ρ < 3.25 KΩcm Inner Tracker (HPK) 3.5 < ρ < 7.5 KΩcm Outer Tracker (STM) Diode Depletion Voltage vs Production Time (HPK) HPK Allowed resistivity range Agreement with HPK: o Deliver all sensors with bulk resistivity within the allowed range o Choose the wafers with lower resistivity for the sensor types that will be mounted in the inner layers Limit corresponding to 3.25 KΩcm RD03 Process Quality Control for the CMS SST Anna Macchiolo 13 Year x week of production

14 Aluminum resistivity Aluminum Surface Resistivity (STM) We measure the Al surface resistivity using long and narrow metal strips implanted directly on the n bulk. The resistance of the Al layer deposited on top of the strips is a parameter that contributes to the input noise seen by the front-end electronics. At the beginning of STM production the surface resistivity was exceeding our specifications (ρ Al < 30 m Ω square ) An increase in the Aluminum implant depth from 1.2 to 2.0 µm solved the problem. Structures/ bin Structures/ bin STM before May 2002 Mean value = 28 m Ω square ρ Al (mω square) STM after May 2002 Mean value = 19 m Ω square ρ Al (mω square) RD03 Process Quality Control for the CMS SST Anna Macchiolo 14

15 Mini-Sensor Breakdown Voltage Breakdown voltage of the mini-sensor Quality Test Centers perform IV on the sensors up to 550 V The mini-sensor in the Standard Moon has the same design characteristics as the fullsize sensors Most of mini-sensors 95 % for STM 98 % for HPK show no sign of breakdown (defined by I > 10 µ A) up to 700 V, where we stop the measurement Structures/ bin Structures/ bin Mini-sensor breakdown voltage (V) STM HPK Mini-sensor breakdown voltage (V) RD03 Process Quality Control for the CMS SST Anna Macchiolo 15

16 Inter-strip Capacitance Inter-strip Capacitance vs Production Time The inter-strip capacitance (C int ) is measured excluding the contribution of the second neighbor strips It depends on the strip pitch and width. In the case of our test-structures (strip width = 30 µm and pitch = 120 µm ) we expect C int around 0.8 pf per cm. This is a typical value also for the full-size sensors A good stability in time is observed both for HPK and STM Inter-strip Capacitance (pf) High values of C int corresponding to batches rejected due to high Vfb Inter-strip capacitance allowed range STM Year x week of production RD03 Process Quality Control for the CMS SST Anna Macchiolo 16

17 Conclusions A working system has been developed to monitor the fabrication process for the CMS SST sensors. We have proved efficient to recognize problems as soon as they appeared (Aluminum resistivity, bulk resistivity, Flat Band Voltage). The collaboration with the two manufacturer companies has allowed us to solve these problems without affecting sensibly the sensor production. Many more hundreds of test-structures ahead of us RD03 Process Quality Control for the CMS SST Anna Macchiolo 17

18 Surface Current vs Flat Band Voltage Flat Band Voltage (V) Back-up 1 RD03 Process Quality Control for the CMS SST Anna Macchiolo 18 Surface current (pa) STM

19 Back-up 2 p + -implant surface resistivity Acceptance interval for p + -implant surface resistivity : 0 < ρ < 400 Ω square HPK STM Ω square Ω square HPK STM Acceptance interval for poly-silicon bias resistors : 1 < ρ < 2 GΩ GΩ Poly-silicon resistor value GΩ RD03 Process Quality Control for the CMS SST Anna Macchiolo 19

20 Back-up 3 Inter-strip resistance Measured among one central strip and the two neighboring ones. The strips are DC coupled and without poly-silicon bias resistors. Acceptance interval for inter-strip resistance : Rpoly > 1 G Ω HPK STM GΩ RD03 Process Quality Control for the CMS SST Anna Macchiolo 20 GΩ

Charge Collection and Capacitance-Voltage analysis in irradiated n-type magnetic Czochralski silicon detectors

Charge Collection and Capacitance-Voltage analysis in irradiated n-type magnetic Czochralski silicon detectors Charge Collection and Capacitance-Voltage analysis in irradiated n-type magnetic Czochralski silicon detectors M. K. Petterson, H.F.-W. Sadrozinski, C. Betancourt SCIPP UC Santa Cruz, 1156 High Street,

More information

Capacitance of the GLAST Prototype Detectors

Capacitance of the GLAST Prototype Detectors SCIPP 96/75 July 1996 Capacitance of the GLAST Prototype Detectors Chastity Bedonie, Zach Dick, Robert Johnson U.C. Santa Cruz 9 July, 1996 About 40 single-sided silicon microstrip detectors of 500 µm

More information

CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland Available on CMS information server CMS NOTE 199/11 The Compact Muon Solenoid Experiment CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 11 February 199 Temperature dependence of the

More information

Mara Bruzzi INFN and University of Florence, Italy and SCIPP, UC Santa Cruz, USA

Mara Bruzzi INFN and University of Florence, Italy and SCIPP, UC Santa Cruz, USA SCIPP 06/16 September 2006 Capacitance-Voltage analysis at different temperatures in heavily irradiated silicon detectors Mara Bruzzi INFN and University of Florence, Italy and SCIPP, UC Santa Cruz, USA

More information

ECE 340 Lecture 39 : MOS Capacitor II

ECE 340 Lecture 39 : MOS Capacitor II ECE 340 Lecture 39 : MOS Capacitor II Class Outline: Effects of Real Surfaces Threshold Voltage MOS Capacitance-Voltage Analysis Things you should know when you leave Key Questions What are the effects

More information

Aspects of radiation hardness for silicon microstrip detectors

Aspects of radiation hardness for silicon microstrip detectors Aspects of radiation hardness for silicon microstrip detectors Richard Wheadon, INFN Pisa, Via Livornese 1291, S. Piero a Grado, Pisa, Italy Abstract The ways in which radiation damage affects the properties

More information

Lecture 12: MOS Capacitors, transistors. Context

Lecture 12: MOS Capacitors, transistors. Context Lecture 12: MOS Capacitors, transistors Context In the last lecture, we discussed PN diodes, and the depletion layer into semiconductor surfaces. Small signal models In this lecture, we will apply those

More information

Development of Radiation Hard Si Detectors

Development of Radiation Hard Si Detectors Development of Radiation Hard Si Detectors Dr. Ajay K. Srivastava On behalf of Detector Laboratory of the Institute for Experimental Physics University of Hamburg, D-22761, Germany. Ajay K. Srivastava

More information

SECTION: Circle one: Alam Lundstrom. ECE 305 Exam 5 SOLUTIONS: Spring 2016 April 18, 2016 M. A. Alam and M.S. Lundstrom Purdue University

SECTION: Circle one: Alam Lundstrom. ECE 305 Exam 5 SOLUTIONS: Spring 2016 April 18, 2016 M. A. Alam and M.S. Lundstrom Purdue University NAME: PUID: SECTION: Circle one: Alam Lundstrom ECE 305 Exam 5 SOLUTIONS: April 18, 2016 M A Alam and MS Lundstrom Purdue University This is a closed book exam You may use a calculator and the formula

More information

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors Lecture 2 Introduction to semiconductors Structures and characteristics in semiconductors Semiconductor p-n junction Metal Oxide Silicon structure Semiconductor contact Literature Glen F. Knoll, Radiation

More information

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors Lecture 2 Introduction to semiconductors Structures and characteristics in semiconductors Semiconductor p-n junction Metal Oxide Silicon structure Semiconductor contact Literature Glen F. Knoll, Radiation

More information

The Silicon-Tungsten Tracker of the DAMPE Mission

The Silicon-Tungsten Tracker of the DAMPE Mission The Silicon-Tungsten Tracker of the DAMPE Mission Philipp Azzarello, DPNC, University of Geneva for the DAMPE-STK collaboration 10th International Hiroshima Symposium on the Development and Application

More information

DEPFET sensors development for the Pixel Detector of BELLE II

DEPFET sensors development for the Pixel Detector of BELLE II DEPFET sensors development for the Pixel Detector of BELLE II 13 th Topical Seminar on Innovative Particle and Radiation Detectors (IPRD13) 7 10 October 2013, Siena, Italy Paola Avella for the DEPFET collaboration

More information

Semiconductor Devices. C. Hu: Modern Semiconductor Devices for Integrated Circuits Chapter 5

Semiconductor Devices. C. Hu: Modern Semiconductor Devices for Integrated Circuits Chapter 5 Semiconductor Devices C. Hu: Modern Semiconductor Devices for Integrated Circuits Chapter 5 Global leader in environmental and industrial measurement Wednesday 3.2. afternoon Tour around facilities & lecture

More information

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors. Fabrication of semiconductor sensor

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors. Fabrication of semiconductor sensor Lecture 2 Introduction to semiconductors Structures and characteristics in semiconductors Semiconductor p-n junction Metal Oxide Silicon structure Semiconductor contact Fabrication of semiconductor sensor

More information

Lecture 0: Introduction

Lecture 0: Introduction Lecture 0: Introduction Introduction q Integrated circuits: many transistors on one chip q Very Large Scale Integration (VLSI): bucketloads! q Complementary Metal Oxide Semiconductor Fast, cheap, low power

More information

Section 12: Intro to Devices

Section 12: Intro to Devices Section 12: Intro to Devices Extensive reading materials on reserve, including Robert F. Pierret, Semiconductor Device Fundamentals Bond Model of Electrons and Holes Si Si Si Si Si Si Si Si Si Silicon

More information

ELEN0037 Microelectronic IC Design. Prof. Dr. Michael Kraft

ELEN0037 Microelectronic IC Design. Prof. Dr. Michael Kraft ELEN0037 Microelectronic IC Design Prof. Dr. Michael Kraft Lecture 2: Technological Aspects Technology Passive components Active components CMOS Process Basic Layout Scaling CMOS Technology Integrated

More information

Characterization of Irradiated Doping Profiles. Wolfgang Treberspurg, Thomas Bergauer, Marko Dragicevic, Manfred Krammer, Manfred Valentan

Characterization of Irradiated Doping Profiles. Wolfgang Treberspurg, Thomas Bergauer, Marko Dragicevic, Manfred Krammer, Manfred Valentan Characterization of Irradiated Doping Profiles, Thomas Bergauer, Marko Dragicevic, Manfred Krammer, Manfred Valentan Vienna Conference on Instrumentation (VCI) 14.02.2013 14.02.2013 2 Content: Experimental

More information

A t XFEL experiment, sensors should have. Capacitance calculations in p + n silicon pixel sensors using three dimensional TCAD simulation approach

A t XFEL experiment, sensors should have. Capacitance calculations in p + n silicon pixel sensors using three dimensional TCAD simulation approach Capacitance calculations in p + n silicon pixel sensors using three dimensional TCAD simulation approach Ajay K. Srivastava a,1 E. Fretwurst a, R.Klanner a a Institute for Experimental Physics, University

More information

Name Class Date. RC Circuit Lab

Name Class Date. RC Circuit Lab RC Circuit Lab Objectives: Students will be able to Use the ScienceWorkshop interface to investigate the relationship between the voltage remaining across a capacitor and the time taken for the discharge

More information

Electrical Characteristics of MOS Devices

Electrical Characteristics of MOS Devices Electrical Characteristics of MOS Devices The MOS Capacitor Voltage components Accumulation, Depletion, Inversion Modes Effect of channel bias and substrate bias Effect of gate oide charges Threshold-voltage

More information

Chapter 13. Capacitors

Chapter 13. Capacitors Chapter 13 Capacitors Objectives Describe the basic structure and characteristics of a capacitor Discuss various types of capacitors Analyze series capacitors Analyze parallel capacitors Analyze capacitive

More information

Ranjeet Dalal, Ashutosh Bhardwaj, Kirti Ranjan, Kavita Lalwani and Geetika Jain

Ranjeet Dalal, Ashutosh Bhardwaj, Kirti Ranjan, Kavita Lalwani and Geetika Jain Simulation of Irradiated Si Detectors, Ashutosh Bhardwaj, Kirti Ranjan, Kavita Lalwani and Geetika Jain CDRST, Department of physics and Astrophysics, University of Delhi, India E-mail: rdalal@cern.ch

More information

EE 434 Lecture 12. Process Flow (wrap up) Device Modeling in Semiconductor Processes

EE 434 Lecture 12. Process Flow (wrap up) Device Modeling in Semiconductor Processes EE 434 Lecture 12 Process Flow (wrap up) Device Modeling in Semiconductor Processes Quiz 6 How have process engineers configured a process to assure that the thickness of the gate oxide for the p-channel

More information

Section 12: Intro to Devices

Section 12: Intro to Devices Section 12: Intro to Devices Extensive reading materials on reserve, including Robert F. Pierret, Semiconductor Device Fundamentals EE143 Ali Javey Bond Model of Electrons and Holes Si Si Si Si Si Si Si

More information

Radiation Effects nm Si 3 N 4

Radiation Effects nm Si 3 N 4 The Active DEPFET Pixel Sensor: Irradiation Effects due to Ionizing Radiation o Motivation / Radiation Effects o Devices and Facilities o Results o Summary and Conclusion MPI Semiconductor Laboratory Munich

More information

Fabrication and Characterization of Al/Al2O3/p-Si MOS Capacitors

Fabrication and Characterization of Al/Al2O3/p-Si MOS Capacitors Fabrication and Characterization of Al/Al2O3/p-Si MOS Capacitors 6 MOS capacitors were fabricated on silicon substrates. ALD deposited Aluminum Oxide was used as dielectric material. Various electrical

More information

Development of a Radiation Hard CMOS Monolithic Pixel Sensor

Development of a Radiation Hard CMOS Monolithic Pixel Sensor Development of a Radiation Hard CMOS Monolithic Pixel Sensor M. Battaglia 1,2, D. Bisello 3, D. Contarato 2, P. Denes 2, D. Doering 2, P. Giubilato 2,3, T.S. Kim 2, Z. Lee 2, S. Mattiazzo 3, V. Radmilovic

More information

Control of Flat Band Voltage by Partial Incorporation of La 2 O 3 or Sc 2 O 3 into HfO 2 in Metal/HfO 2 /SiO 2 /Si MOS Capacitors

Control of Flat Band Voltage by Partial Incorporation of La 2 O 3 or Sc 2 O 3 into HfO 2 in Metal/HfO 2 /SiO 2 /Si MOS Capacitors Control of Flat Band Voltage by Partial Incorporation of La 2 O 3 or Sc 2 O 3 into HfO 2 in Metal/HfO 2 /SiO 2 /Si MOS Capacitors M. Adachi 1, K. Okamoto 1, K. Kakushima 2, P. Ahmet 1, K. Tsutsui 2, N.

More information

6.012 Electronic Devices and Circuits

6.012 Electronic Devices and Circuits Page 1 of 12 YOUR NAME Department of Electrical Engineering and Computer Science Massachusetts Institute of Technology 6.012 Electronic Devices and Circuits FINAL EXAMINATION Open book. Notes: 1. Unless

More information

Semiconductor Detectors are Ionization Chambers. Detection volume with electric field Energy deposited positive and negative charge pairs

Semiconductor Detectors are Ionization Chambers. Detection volume with electric field Energy deposited positive and negative charge pairs 1 V. Semiconductor Detectors V.1. Principles Semiconductor Detectors are Ionization Chambers Detection volume with electric field Energy deposited positive and negative charge pairs Charges move in field

More information

Tracking Detector Material Issues for the slhc

Tracking Detector Material Issues for the slhc Tracking Detector Material Issues for the slhc Hartmut F.-W. Sadrozinski SCIPP, UC Santa Cruz, CA 95064 Hartmut F.-W. Sadrozinski, US ATLAS Upgrade Meeting Nov 10, 2005 1 Outline of the talk - Motivation

More information

Final Examination EE 130 December 16, 1997 Time allotted: 180 minutes

Final Examination EE 130 December 16, 1997 Time allotted: 180 minutes Final Examination EE 130 December 16, 1997 Time allotted: 180 minutes Problem 1: Semiconductor Fundamentals [30 points] A uniformly doped silicon sample of length 100µm and cross-sectional area 100µm 2

More information

Silicon Detectors. Particle Physics

Silicon Detectors. Particle Physics Mitglied der Helmholtz-Gemeinschaft Silicon Detectors for Particle Physics 9. August 2012 Ralf Schleichert, Institut für Kernphysik Outline Different Cameras Silicon Detectors Taking Pictures in Particle

More information

ATL-INDET /04/2000

ATL-INDET /04/2000 Evolution of silicon micro-strip detector currents during proton irradiation at the CERN PS ATL-INDET-2000-009 17/04/2000 R.S.Harper aλ, P.P.Allport b, L.Andricek c, C.M.Buttar a, J.R.Carter d, G.Casse

More information

Chapter 4 Field-Effect Transistors

Chapter 4 Field-Effect Transistors Chapter 4 Field-Effect Transistors Microelectronic Circuit Design Richard C. Jaeger Travis N. Blalock 5/5/11 Chap 4-1 Chapter Goals Describe operation of MOSFETs. Define FET characteristics in operation

More information

MOSFET: Introduction

MOSFET: Introduction E&CE 437 Integrated VLSI Systems MOS Transistor 1 of 30 MOSFET: Introduction Metal oxide semiconductor field effect transistor (MOSFET) or MOS is widely used for implementing digital designs Its major

More information

an introduction to Semiconductor Devices

an introduction to Semiconductor Devices an introduction to Semiconductor Devices Donald A. Neamen Chapter 6 Fundamentals of the Metal-Oxide-Semiconductor Field-Effect Transistor Introduction: Chapter 6 1. MOSFET Structure 2. MOS Capacitor -

More information

Lecture 11: MOS Transistor

Lecture 11: MOS Transistor Lecture 11: MOS Transistor Prof. Niknejad Lecture Outline Review: MOS Capacitors Regions MOS Capacitors (3.8 3.9) CV Curve Threshold Voltage MOS Transistors (4.1 4.3): Overview Cross-section and layout

More information

The Hermes Recoil Silicon Detector

The Hermes Recoil Silicon Detector The Hermes Recoil Silicon Detector Introduction Detector design considerations Silicon detector overview TIGRE microstrip sensors Readout electronics Test beam results Vertex 2002 J. Stewart DESY Zeuthen

More information

Circuits. L5: Fabrication and Layout -2 ( ) B. Mazhari Dept. of EE, IIT Kanpur. B. Mazhari, IITK. G-Number

Circuits. L5: Fabrication and Layout -2 ( ) B. Mazhari Dept. of EE, IIT Kanpur. B. Mazhari, IITK. G-Number EE610: CMOS Analog Circuits L5: Fabrication and Layout -2 (12.8.2013) B. Mazhari Dept. of EE, IIT Kanpur 44 Passive Components: Resistor Besides MOS transistors, sometimes one requires to implement passive

More information

LAYOUT TECHNIQUES. Dr. Ivan Grech

LAYOUT TECHNIQUES. Dr. Ivan Grech LAYOUT TECHNIQUES OUTLINE Transistor Layout Resistor Layout Capacitor Layout Floor planning Mixed A/D Layout Automatic Analog Layout Layout Techniques Main Layers in a typical Double-Poly, Double-Metal

More information

CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland Available on CMS information server CMS NOTE 2001/023 The Compact Muon Solenoid Experiment CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland May 18, 2001 Investigations of operating scenarios

More information

AIDA-2020 Advanced European Infrastructures for Detectors at Accelerators. Conference/Workshop Paper

AIDA-2020 Advanced European Infrastructures for Detectors at Accelerators. Conference/Workshop Paper AIDA-2020-CONF-2016-007 AIDA-2020 Advanced European Infrastructures for Detectors at Accelerators Conference/Workshop Paper Measurements and TCAD Simulations of Bulk and Surface Radiation Damage Effects

More information

Semiconductor-Detectors

Semiconductor-Detectors Semiconductor-Detectors 1 Motivation ~ 195: Discovery that pn-- junctions can be used to detect particles. Semiconductor detectors used for energy measurements ( Germanium) Since ~ 3 years: Semiconductor

More information

RD50 Recent Results - Development of radiation hard sensors for SLHC

RD50 Recent Results - Development of radiation hard sensors for SLHC - Development of radiation hard sensors for SLHC Anna Macchiolo Max-Planck-Institut für Physik Föhringer Ring 6, Munich, Germany E-mail: Anna.Macchiolo@mppmu.mpg.de on behalf of the RD50 Collaboration

More information

Fig. 1. Two common types of van der Pauw samples: clover leaf and square. Each sample has four symmetrical electrical contacts.

Fig. 1. Two common types of van der Pauw samples: clover leaf and square. Each sample has four symmetrical electrical contacts. 15 2. Basic Electrical Parameters of Semiconductors: Sheet Resistivity, Resistivity and Conduction Type 2.1 Objectives 1. Familiarizing with experimental techniques used for the measurements of electrical

More information

nmos IC Design Report Module: EEE 112

nmos IC Design Report Module: EEE 112 nmos IC Design Report Author: 1302509 Zhao Ruimin Module: EEE 112 Lecturer: Date: Dr.Zhao Ce Zhou June/5/2015 Abstract This lab intended to train the experimental skills of the layout designing of the

More information

X-ray induced radiation damage in segmented p + n silicon sensors

X-ray induced radiation damage in segmented p + n silicon sensors in segmented p + n silicon sensors Jiaguo Zhang, Eckhart Fretwurst, Robert Klanner, Joern Schwandt Hamburg University, Germany E-mail: jiaguo.zhang@desy.de Deutsches Elektronen-Synchrotron (DESY), Germany

More information

Lecture 8. Detectors for Ionizing Particles

Lecture 8. Detectors for Ionizing Particles Lecture 8 Detectors for Ionizing Particles Content Introduction Overview of detector systems Sources of radiation Radioactive decay Cosmic Radiation Accelerators Interaction of Radiation with Matter General

More information

CIRCUIT ELEMENT: CAPACITOR

CIRCUIT ELEMENT: CAPACITOR CIRCUIT ELEMENT: CAPACITOR PROF. SIRIPONG POTISUK ELEC 308 Types of Circuit Elements Two broad types of circuit elements Ati Active elements -capable of generating electric energy from nonelectric energy

More information

Characterisation of silicon sensor materials and designs for the CMS Tracker Upgrade

Characterisation of silicon sensor materials and designs for the CMS Tracker Upgrade Characterisation of silicon sensor materials and designs for the CMS Tracker Upgrade KIT - Karlsruhe Institute of Technology (DE) E-mail: alexander.dierlamm@cern.ch During the high luminosity phase of

More information

MOS Capacitors ECE 2204

MOS Capacitors ECE 2204 MOS apacitors EE 2204 Some lasses of Field Effect Transistors Metal-Oxide-Semiconductor Field Effect Transistor MOSFET, which will be the type that we will study in this course. Metal-Semiconductor Field

More information

The ATLAS Silicon Microstrip Tracker

The ATLAS Silicon Microstrip Tracker 9th 9th Topical Seminar on Innovative Particle and Radiation Detectors 23-26 May 2004 Siena3 The ATLAS Silicon Microstrip Tracker Zdenek Dolezal, Charles University at Prague, for the ATLAS SCT Collaboration

More information

Integrated Circuits & Systems

Integrated Circuits & Systems Federal University of Santa Catarina Center for Technology Computer Science & Electronics Engineering Integrated Circuits & Systems INE 5442 Lecture 7 Interconnections 1: wire resistance, capacitance,

More information

Exercise 1: Capacitors

Exercise 1: Capacitors Capacitance AC 1 Fundamentals Exercise 1: Capacitors EXERCISE OBJECTIVE When you have completed this exercise, you will be able to describe the effect a capacitor has on dc and ac circuits by using measured

More information

Carbon Nanotubes in Interconnect Applications

Carbon Nanotubes in Interconnect Applications Carbon Nanotubes in Interconnect Applications Page 1 What are Carbon Nanotubes? What are they good for? Why are we interested in them? - Interconnects of the future? Comparison of electrical properties

More information

Epitaxial SiC Schottky barriers for radiation and particle detection

Epitaxial SiC Schottky barriers for radiation and particle detection Epitaxial SiC Schottky barriers for radiation and particle detection M. Bruzzi, M. Bucciolini, R. D'Alessandro, S. Lagomarsino, S. Pini, S. Sciortino INFN Firenze - Università di Firenze F. Nava INFN Bologna

More information

Status Report: Charge Cloud Explosion

Status Report: Charge Cloud Explosion Status Report: Charge Cloud Explosion J. Becker, D. Eckstein, R. Klanner, G. Steinbrück University of Hamburg Detector laboratory 1. Introduction and Motivation. Set-up available for measurement 3. Measurements

More information

Guard Ring Width Impact on Impact Parameter Performances and Structure Simulations

Guard Ring Width Impact on Impact Parameter Performances and Structure Simulations LHCb-2003-034, VELO Note 13th May 2003 Guard Ring Width Impact on Impact Parameter Performances and Structure Simulations authors A Gouldwell, C Parkes, M Rahman, R Bates, M Wemyss, G Murphy The University

More information

Department of Electrical and Computer Engineering, Cornell University. ECE 3150: Microelectronics. Spring Due on March 01, 2018 at 7:00 PM

Department of Electrical and Computer Engineering, Cornell University. ECE 3150: Microelectronics. Spring Due on March 01, 2018 at 7:00 PM Department of Electrical and Computer Engineering, Cornell University ECE 3150: Microelectronics Spring 2018 Homework 4 Due on March 01, 2018 at 7:00 PM Suggested Readings: a) Lecture notes Important Note:

More information

MICRO-SCALE SHEET RESISTANCE MEASUREMENTS ON ULTRA SHALLOW JUNCTIONS

MICRO-SCALE SHEET RESISTANCE MEASUREMENTS ON ULTRA SHALLOW JUNCTIONS MICRO-SCALE SHEET RESISTANCE MEASUREMENTS ON ULTRA SHALLOW JUNCTIONS Christian L. Petersen, Rong Lin, Dirch H. Petersen, Peter F. Nielsen CAPRES A/S, Burnaby, BC, Canada CAPRES A/S, Lyngby, Denmark We

More information

Low-Cost Capacitance Profiling of a Semiconductor

Low-Cost Capacitance Profiling of a Semiconductor Low-Cost Capacitance Profiling of a Semiconductor Contact Information John Essick Reed College Department of Physics 3203 SE Woodstock Blvd. Portland, Oregon 97202 USA telephone:(503) 517-7841 email: jessick@reed.edu

More information

CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland Available on CMS information server CMS NOTE 1996/005 The Compact Muon Solenoid Experiment CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland Performance of the Silicon Detectors for the

More information

D. Meier. representing the RD42 Collaboration. Bristol University, CERN, CPP Marseille, Lawrence Livermore National Lab, LEPSI

D. Meier. representing the RD42 Collaboration. Bristol University, CERN, CPP Marseille, Lawrence Livermore National Lab, LEPSI Diamond as a Particle Detector D. Meier representing the RD42 Collaboration Bristol University, CERN, CPP Marseille, Lawrence Livermore National Lab, LEPSI Strasbourg, Los Alamos National Lab, MPIK Heidelberg,

More information

ECE 305 Exam 5 SOLUTIONS: Spring 2015 April 17, 2015 Mark Lundstrom Purdue University

ECE 305 Exam 5 SOLUTIONS: Spring 2015 April 17, 2015 Mark Lundstrom Purdue University NAME: PUID: : ECE 305 Exam 5 SOLUTIONS: April 17, 2015 Mark Lundstrom Purdue University This is a closed book exam. You may use a calculator and the formula sheet at the end of this exam. Following the

More information

QTC Pisa up-date. STM & HPK Sensors received from : December 03-February. 04 Qualification Summary and preliminary acceptance Company data comparison

QTC Pisa up-date. STM & HPK Sensors received from : December 03-February. 04 Qualification Summary and preliminary acceptance Company data comparison QTC Pisa up-date STM & HPK Sensrs received frm : December 03-February 04 Qualificatin Summary and preliminary acceptance Cmpany data cmparisn L.Brrell, D.Kartashv, A.Messine, G.Segneri, D.Sentenac March

More information

Device Models (PN Diode, MOSFET )

Device Models (PN Diode, MOSFET ) Device Models (PN Diode, MOSFET ) Instructor: Steven P. Levitan steve@ece.pitt.edu TA: Gayatri Mehta, José Martínez Book: Digital Integrated Circuits: A Design Perspective; Jan Rabaey Lab Notes: Handed

More information

General Physics (PHY 2140)

General Physics (PHY 2140) General Physics (PHY 2140) Lecture 7 Electrostatics and electrodynamics Capacitance and capacitors capacitors with dielectrics Electric current current and drift speed resistance and Ohm s law http://www.physics.wayne.edu/~apetrov/phy2140/

More information

MOS CAPACITOR AND MOSFET

MOS CAPACITOR AND MOSFET EE336 Semiconductor Devices 1 MOS CAPACITOR AND MOSFET Dr. Mohammed M. Farag Ideal MOS Capacitor Semiconductor Devices Physics and Technology Chapter 5 EE336 Semiconductor Devices 2 MOS Capacitor Structure

More information

Radiation damage models: comparison between Silvaco and Synopsys

Radiation damage models: comparison between Silvaco and Synopsys Radiation damage models: comparison between Silvaco and Synopsys J. Beyer a), M. Bomben b), A. Macchiolo a), R. Nisius a) a) Max Planck Institut für Physik, München b) LPNHE & Université Paris Diderot,

More information

Technology Brief 9: Capacitive Sensors

Technology Brief 9: Capacitive Sensors 218 TEHNOLOGY BRIEF 9: APAITIVE SENSORS Technology Brief 9: apacitive Sensors To sense is to respond to a stimulus. (See Tech Brief 7 on resistive sensors.) A capacitor can function as a sensor if the

More information

First Results and Realization Status of a Proton Computed Radiography Device

First Results and Realization Status of a Proton Computed Radiography Device First Results and Realization Status of a Proton Computed Radiography Device V. Sipala for the PRIMA collaboration V.Sipalaa,b, D.LoPrestia,b, N.Randazzob, M.Bruzzid,e, D.Menichellie,d, C.Civininid, M.Bucciolinic,d,

More information

physics/ Sep 1997

physics/ Sep 1997 GLAS-PPE/97-6 28 August 1997 Department of Physics & Astronomy Experimental Particle Physics Group Kelvin Building, University of Glasgow, Glasgow, G12 8QQ, Scotland. Telephone: +44 - ()141 3398855 Fax:

More information

Recent B Physics Results and Silicon Detector Longevity Studies from CDF

Recent B Physics Results and Silicon Detector Longevity Studies from CDF Recent B Physics Results and Silicon Detector Longevity Studies from CDF Contents CDF Silicon Detectors: Preparedness for the proposed Run III Radiation ageing of the sensors Recent B Physics Results:

More information

6.012 Electronic Devices and Circuits

6.012 Electronic Devices and Circuits Page 1 of 10 YOUR NAME Department of Electrical Engineering and Computer Science Massachusetts Institute of Technology 6.012 Electronic Devices and Circuits Exam No. 2 Thursday, November 5, 2009 7:30 to

More information

EE 560 MOS TRANSISTOR THEORY

EE 560 MOS TRANSISTOR THEORY 1 EE 560 MOS TRANSISTOR THEORY PART 1 TWO TERMINAL MOS STRUCTURE V G (GATE VOLTAGE) 2 GATE OXIDE SiO 2 SUBSTRATE p-type doped Si (N A = 10 15 to 10 16 cm -3 ) t ox V B (SUBSTRATE VOLTAGE) EQUILIBRIUM:

More information

EE 434 Lecture 13. Basic Semiconductor Processes Devices in Semiconductor Processes

EE 434 Lecture 13. Basic Semiconductor Processes Devices in Semiconductor Processes EE 434 Lecture 3 Basic Semiconductor Processes Devices in Semiconductor Processes Quiz 9 The top view of a device fabricated in a bulk CMOS process is shown in the figure below a) Identify the device b)

More information

Components of a generic collider detector

Components of a generic collider detector Lecture 24 Components of a generic collider detector electrons - ionization + bremsstrahlung photons - pair production in high Z material charged hadrons - ionization + shower of secondary interactions

More information

Low Power VLSI Circuits and Systems Prof. Ajit Pal Department of Computer Science and Engineering Indian Institute of Technology, Kharagpur

Low Power VLSI Circuits and Systems Prof. Ajit Pal Department of Computer Science and Engineering Indian Institute of Technology, Kharagpur Low Power VLSI Circuits and Systems Prof. Ajit Pal Department of Computer Science and Engineering Indian Institute of Technology, Kharagpur Lecture No. # 08 MOS Inverters - III Hello, and welcome to today

More information

Lecture 4: CMOS Transistor Theory

Lecture 4: CMOS Transistor Theory Introduction to CMOS VLSI Design Lecture 4: CMOS Transistor Theory David Harris, Harvey Mudd College Kartik Mohanram and Steven Levitan University of Pittsburgh Outline q Introduction q MOS Capacitor q

More information

Dr. Maria-Alexandra PAUN

Dr. Maria-Alexandra PAUN Performance comparison of Hall Effect Sensors obtained by regular bulk or SOI CMOS technology Dr. Maria-Alexandra PAUN Visiting Researcher High Voltage Microelectronics and Sensors (HVMS) Group, Department

More information

EECS130 Integrated Circuit Devices

EECS130 Integrated Circuit Devices EECS130 Integrated Circuit Devices Professor Ali Javey 10/02/2007 MS Junctions, Lecture 2 MOS Cap, Lecture 1 Reading: finish chapter14, start chapter16 Announcements Professor Javey will hold his OH at

More information

JFET/MESFET. JFET: small gate current (reverse leakage of the gate-to-channel junction) More gate leakage than MOSFET, less than bipolar.

JFET/MESFET. JFET: small gate current (reverse leakage of the gate-to-channel junction) More gate leakage than MOSFET, less than bipolar. JFET/MESFET JFET: small gate current (reverse leakage of the gate-to-channel junction) More gate leakage than MOSFET, less than bipolar. JFET has higher transconductance than the MOSFET. Used in low-noise,

More information

Lecture 150 Basic IC Processes (10/10/01) Page ECE Analog Integrated Circuits and Systems P.E. Allen

Lecture 150 Basic IC Processes (10/10/01) Page ECE Analog Integrated Circuits and Systems P.E. Allen Lecture 150 Basic IC Processes (10/10/01) Page 1501 LECTURE 150 BASIC IC PROCESSES (READING: TextSec. 2.2) INTRODUCTION Objective The objective of this presentation is: 1.) Introduce the fabrication of

More information

Homework #1 - September 9, Due: September 16, 2005 at recitation ( 2 PM latest) (late homework will not be accepted)

Homework #1 - September 9, Due: September 16, 2005 at recitation ( 2 PM latest) (late homework will not be accepted) Fall 2005 6.012 Microelectronic Devices and Circuits Prof. J. A. del Alamo Homework #1 - September 9, 2005 Due: September 16, 2005 at recitation ( 2 PM latest) (late homework will not be accepted) Please

More information

ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems

ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Lec 6: September 14, 2015 MOS Model You are Here: Transistor Edition! Previously: simple models (0 and 1 st order) " Comfortable

More information

REVISED HIGHER PHYSICS REVISION BOOKLET ELECTRONS AND ENERGY

REVISED HIGHER PHYSICS REVISION BOOKLET ELECTRONS AND ENERGY REVSED HGHER PHYSCS REVSON BOOKLET ELECTRONS AND ENERGY Kinross High School Monitoring and measuring a.c. Alternating current: Mains supply a.c.; batteries/cells supply d.c. Electrons moving back and forth,

More information

Solid State Detectors Semiconductor detectors Halbleiterdetektoren

Solid State Detectors Semiconductor detectors Halbleiterdetektoren Solid State Detectors Semiconductor detectors Halbleiterdetektoren Doris Eckstein DESY Where are solid state detectors used? > Nuclear Physics: Energy measurement of charged particles (particles up to

More information

Semiconductor Detectors

Semiconductor Detectors Semiconductor Detectors Summary of Last Lecture Band structure in Solids: Conduction band Conduction band thermal conductivity: E g > 5 ev Valence band Insulator Charge carrier in conductor: e - Charge

More information

Lecture 04 Review of MOSFET

Lecture 04 Review of MOSFET ECE 541/ME 541 Microelectronic Fabrication Techniques Lecture 04 Review of MOSFET Zheng Yang (ERF 3017, email: yangzhen@uic.edu) What is a Transistor? A Switch! An MOS Transistor V GS V T V GS S Ron D

More information

Lecture 15 OUTLINE. MOSFET structure & operation (qualitative) Review of electrostatics The (N)MOS capacitor

Lecture 15 OUTLINE. MOSFET structure & operation (qualitative) Review of electrostatics The (N)MOS capacitor Lecture 15 OUTLINE MOSFET structure & operation (qualitative) Review of electrostatics The (N)MOS capacitor Electrostatics t ti Charge vs. voltage characteristic Reading: Chapter 6.1 6.2.1 EE105 Fall 2007

More information

Author s Accepted Manuscript

Author s Accepted Manuscript Author s Accepted Manuscript Simulation of electrical parameters of new design of SLHC silicon sensors for large radii O. Militaru, T. Bergauer, M. Bergholz, P. Blüm, W. de Boer, K. Borras, E. Cortina

More information

Lab 5 - Capacitors and RC Circuits

Lab 5 - Capacitors and RC Circuits Lab 5 Capacitors and RC Circuits L51 Name Date Partners Lab 5 Capacitors and RC Circuits OBJECTIVES To define capacitance and to learn to measure it with a digital multimeter. To explore how the capacitance

More information

EE130: Integrated Circuit Devices

EE130: Integrated Circuit Devices EE130: Integrated Circuit Devices (online at http://webcast.berkeley.edu) Instructor: Prof. Tsu-Jae King (tking@eecs.berkeley.edu) TA s: Marie Eyoum (meyoum@eecs.berkeley.edu) Alvaro Padilla (apadilla@eecs.berkeley.edu)

More information

EE105 - Fall 2006 Microelectronic Devices and Circuits

EE105 - Fall 2006 Microelectronic Devices and Circuits EE105 - Fall 2006 Microelectronic Devices and Circuits Prof. Jan M. Rabaey (jan@eecs) Lecture 7: MOS Transistor Some Administrative Issues Lab 2 this week Hw 2 due on We Hw 3 will be posted same day MIDTERM

More information

Semiconductor X-Ray Detectors. Tobias Eggert Ketek GmbH

Semiconductor X-Ray Detectors. Tobias Eggert Ketek GmbH Semiconductor X-Ray Detectors Tobias Eggert Ketek GmbH Semiconductor X-Ray Detectors Part A Principles of Semiconductor Detectors 1. Basic Principles 2. Typical Applications 3. Planar Technology 4. Read-out

More information

ECEN 3320 Semiconductor Devices Final exam - Sunday December 17, 2000

ECEN 3320 Semiconductor Devices Final exam - Sunday December 17, 2000 Your Name: ECEN 3320 Semiconductor Devices Final exam - Sunday December 17, 2000 1. Review questions a) Illustrate the generation of a photocurrent in a p-n diode by drawing an energy band diagram. Indicate

More information

Class 05: Device Physics II

Class 05: Device Physics II Topics: 1. Introduction 2. NFET Model and Cross Section with Parasitics 3. NFET as a Capacitor 4. Capacitance vs. Voltage Curves 5. NFET as a Capacitor - Band Diagrams at V=0 6. NFET as a Capacitor - Accumulation

More information