The New Single-silicon TFTs Structure for Kink- current Suppression with Symmetric Dual-Gate by Three Split Floating N+ Zones Dept. of Electrical Engineering,

Slides:



Advertisements
Similar presentations
Lecture Metal-Oxide-Semiconductor (MOS) Field-Effect Transistors (FET) MOSFET Introduction 1.
Advertisements

ECA1212 Introduction to Electrical & Electronics Engineering Chapter 6: Field Effect Transistor by Muhazam Mustapha, October 2011.
SOGANG UNIVERSITY SOGANG UNIVERSITY. SEMICONDUCTOR DEVICE LAB. Power MOSFETs SD Lab. SOGANG Univ. Doohyung Cho.
SOGANG UNIVERSITY SOGANG UNIVERSITY. SEMICONDUCTOR DEVICE LAB. Introduction SD Lab. SOGANG Univ. Gil Yong Song.
J-FET (Junction Field Effect Transistor) Introduction The field-effect transistor (FET) controls the current between two points but does so differently.
Semiconductor basics 1. Vacuum tubes  Diode  Triode 2. Semiconductors  Diode  Transistors Bipolar Bipolar Field Effect Field Effect 3. What’s next?
MOSFETs Monday 19 th September. MOSFETs Monday 19 th September In this presentation we will look at the following: State the main differences between.
Department of Aeronautics and Astronautics NCKU Nano and MEMS Technology LAB. 1 Chapter IV June 14, 2015June 14, 2015June 14, 2015 P-n Junction.
Lecture 2: CMOS Transistor Theory
Spring 2007EE130 Lecture 38, Slide 1 Lecture #38 OUTLINE The MOSFET: Bulk-charge theory Body effect parameter Channel length modulation parameter PMOSFET.
VLSI design Lecture 1: MOS Transistor Theory. CMOS VLSI Design3: CMOS Transistor TheorySlide 2 Outline  Introduction  MOS Capacitor  nMOS I-V Characteristics.
Lecture 19 OUTLINE The MOSFET: Structure and operation
Dr. Nasim Zafar Electronics 1 EEE 231 – BS Electrical Engineering Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
ECE 342 – Jose Schutt-Aine 1 ECE 342 Solid-State Devices & Circuits 6. Bipolar Transistors Jose E. Schutt-Aine Electrical & Computer Engineering University.
Lecture 3: CMOS Transistor Theory
© The McGraw-Hill Companies, Inc McGraw-Hill 1 PRINCIPLES AND APPLICATIONS OF ELECTRICAL ENGINEERING THIRD EDITION G I O R G I O R I Z Z O N I 9.
Chapter 6 Field Effect Transistors 6.1 Transistor Operation 6.2 The Junction FET 6.3 The Metal-Semiconductor FET 6.4 The Metal-Insulator-Semiconductor.
EEE1012 Introduction to Electrical & Electronics Engineering Chapter 7: Field Effect Transistor by Muhazam Mustapha, October 2010.
Norhayati Soin 06 KEEE 4426 WEEK 7/1 6/02/2006 CHAPTER 2 WEEK 7 CHAPTER 2 MOSFETS I-V CHARACTERISTICS CHAPTER 2.
SOGANG UNIVERSITY SOGANG UNIVERSITY. SEMICONDUCTOR DEVICE LAB. Bipolar Junction Transistor (1) SD Lab. SOGANG Univ. BYUNGSOO KIM.
EXAMPLE 6.1 OBJECTIVE Fp = 0.288 V
ECE340 ELECTRONICS I MOSFET TRANSISTORS AND AMPLIFIERS.
Short Channel Effects in MOSFET
InAs Inserted HEMT 연성진.
Field Effect Transistors
Vanderbilt MURI meeting, June 14 th &15 th 2007 Band-To-Band Tunneling (BBT) Induced Leakage Current Enhancement in Irradiated Fully Depleted SOI Devices.
IEEE’s Hands on Practical Electronics (HOPE) Lesson 8: Transistors.
Semiconductor Devices Lecture 5, pn-Junction Diode
President UniversityErwin SitompulSDP 8/1 Dr.-Ing. Erwin Sitompul President University Lecture 8 Semiconductor Device Physics
Conductors – many electrons free to move
1 Concepts of electrons and holes in semiconductors.
Introduction to semiconductor technology. Outline –7 Field effect transistors MOS transistor ”current equation" MOS transistor channel mobility Substrate.
HO #3: ELEN Review MOS TransistorsPage 1S. Saha Long Channel MOS Transistors The theory developed for MOS capacitor (HO #2) can be directly extended.
CMOS VLSI Design CMOS Transistor Theory
Introduction to CMOS VLSI Design Lecture 4: CMOS Transistor Theory David Harris Harvey Mudd College Spring 2007.
1 Other Transistor Topologies 30 March and 1 April 2015 The two gate terminals are tied together to form single gate connection; the source terminal is.
Ulrich Abelein, Mathias Born, Markus Schindler, Andreas Assmuth, Peter Iskra, Torsten Sulima, Ignaz Eisele Doping Profile Dependence of the Vertical Impact.
Source-gated Transistor Seokmin Hong. Why do we need it? * Short Channel Effects Source/Drain Charge Sharing Drain-Induced Barrier Lowering Subsurface.
Introduction to semiconductor technology. Outline –6 Junctions Metal-semiconductor junctions –6 Field effect transistors JFET and MOS transistors Ideal.
Nano and Giga Challenges in Microelectronics Symposium and Summer School Research and Development Opportunities Cracow Sep , 2004 Afternoon 11: Nanotechnology.
Principles of Semiconductor Devices ( 집적 회로 소자 ) Principles of Semiconductor Devices ( 집적 회로 소자 ) Hanyang University Division of Electronics & Computer.
1 Concepts of electrons and holes in semiconductors.
Univ. of Inchon 6 pn Junction Diode : I-V Characteristics 반도체 소자 연구실 박 종 태
CMOS VLSI Design 4th Ed. EEL 6167: VLSI Design Wujie Wen, Assistant Professor Department of ECE Lecture 3A: CMOs Transistor Theory Slides adapted from.
ELECTRONICS II VLSI DESIGN FALL 2013 LECTURE 5 INSTRUCTOR: L.M. HEAD, PhD ELECTRICAL & COMPUTER ENGINEERING ROWAN UNIVERSITY.
UNIT II : BASIC ELECTRICAL PROPERTIES
J-FET (Junction Field Effect Transistor)
Other Transistor Topologies
VLSI design Short channel Effects in Deep Submicron CMOS
Intro to Semiconductors and p-n junction devices
Device Structure & Simulation
ELECTRONICS AND COMMUNICATION
3: CMOS Transistor Theory
5.4 Reverse-Bias Breakdown
6.3.3 Short Channel Effects When the channel length is small (less than 1m), high field effect must be considered. For Si, a better approximation of field-dependent.
VLSI System Design Lect. 2.1 CMOS Transistor Theory
Lecture 19 OUTLINE The MOSFET: Structure and operation
Reading: Finish Chapter 17,
Sung June Kim Chapter 19. MODERN FET STRUCTURES Sung June Kim
Short channel effects Zewei Ding.
Prof. Hsien-Hsin Sean Lee
Semiconductor devices and physics
Lecture 3 OUTLINE Semiconductor Basics (cont’d) PN Junction Diodes
Lecture 3: CMOS Transistor Theory
EXAMPLE 7.1 BJECTIVE Determine the total bias current on an IC due to subthreshold current. Assume there are 107 n-channel transistors on a single chip,
Lecture 3: CMOS Transistor Theory
Lecture 3: CMOS Transistor Theory
JFET Junction Field Effect Transistor.
Solid State Electronics ECE-1109
Other Transistor Topologies
Presentation transcript:

The New Single-silicon TFTs Structure for Kink- current Suppression with Symmetric Dual-Gate by Three Split Floating N+ Zones Dept. of Electrical Engineering, Korea Univ. Dae Yeon Lee Supervised by Man Young Sung (Korea Univ.)

Semiconductor & CAD Lab. Dae Yeon Lee 2 Contents Introduction Background Proposal Simulation & Results Conclusion

Semiconductor & CAD Lab. Dae Yeon Lee 3 Introduction  The Conventional Single-Gate TFT * High On-current * High Electric Field at the Channel/Drain Junction * Kink-Effect Premature Breakdown !  The Conventional Dual-Gate TFT * Low On-current * Low Electric Field at the Channel/Drain Junction * Stable I-V Characteristic by Kink-Effect Suppression Goal is the Mixing of The Merit the each two TFTs 1. Kink-Effect Suppression 2. Improved On-Current High On-Current Reduction of Kink-Effect +

Semiconductor & CAD Lab. Dae Yeon Lee 4 Back Ground  Lowering the Electric Field by having Dual-Gate Structure Lowering the Impact Ionization at the Channel/Drain Junction Lowering the Generated Holes flowed to Source/Channel Junction Floating N+ region recombines with the Holes Defense the lowering the Electrostatic Potential Barrier at the Source/Channel Junction by the Holes Proposed TFT structure achieved the reduction of the Kink-Effect so that stable Drain Current in the Saturation Region Defense PBT action Parasitic Bipolar Transistor

Semiconductor & CAD Lab. Dae Yeon Lee 5 Proposal  The Dual-Gate TFT with Floating N+ channel oxide Gate SourceDrain N+ 16um 400nm 3um 100nm 1um 1.65um Mo 1um 1.65um 0.7um 700nm 110nm N+ 2um Total channel length=10um 400nm P P PP N+ - Off-Set Region Electrons inject at the Forward Bias Middle N+ region length < 1.51 um Lowering the Electric Field

Semiconductor & CAD Lab. Dae Yeon Lee 6  Design Rules

Semiconductor & CAD Lab. Dae Yeon Lee 7 Simulation & Results  Electrostatic Potential  Hole concentration  Electric Field  Drain Current – Drain Voltage Output Characteristics  Output Conductance

Semiconductor & CAD Lab. Dae Yeon Lee 8  Electrostatic Potential Conventional Dual-gate TFT Proposed Dual-gate TFT Conventional Single-gate TFT V G = 7 V, V D = 12 V  Lowering potential barrier at the source causes the kink effect.  Proposed TFT’s potential barrier enhanced the potential barrier 5 times than Single - gate TFT and enhanced 18 % that of conventional dual-gate TFT.

Semiconductor & CAD Lab. Dae Yeon Lee 9  Electrostatic Potential (Zoom In) V G = 7 V, V D = 12 V  The channel region starts from 4.3 um point  The Potential Barrier value for the each TFTs Value is 0.5 V, 2.3 V, 2.8 V at a 5 um point which starts floating n+ region Source Channel

Semiconductor & CAD Lab. Dae Yeon Lee 10  Hole Concentration Conventional Single-gate TFT Conventional Dual-gate TFT Proposed Dual-gate TFT >  High Electric field at Drain Junction causes Impact Ionization so that holes flow to the source junction through channel -> PBT action  Floating N + regions recombine with holes so that hole concentration at the source junction can be reduce. V G = 7 V, V D = 12 V

Semiconductor & CAD Lab. Dae Yeon Lee 11  Hole Concentration (Zoom In) V G = 7 V, V D = 12 V  The channel region starts from 4.3 um point  The Hole concentration value for the each TFTs Value is /cm 3, 10 1 /cm 3, /cm 3 at a 5 um point which starts floating n+ region Source Channel

Semiconductor & CAD Lab. Dae Yeon Lee 12  Electric Field Conventional Single-gate TFT Conventional Dual-gate TFT Proposed Dual-gate TFT  High Electric field at Drain Junction causes kink effect.  The usual approach to reduce this effect is to limit the impact ionization contribution decreasing the electric field at the drain junction. V G = 7 V, V D = 12 V

Semiconductor & CAD Lab. Dae Yeon Lee 13  Electric Field (Zoom In) V G = 7 V, V D = 12 V  The channel region starts from 12.9 um point  The electric field value of each TFT is approximately 10 5 V, 2.8×10 2 V, and 2.9×10 2 V. Channel Drain

Semiconductor & CAD Lab. Dae Yeon Lee 14  Drain Current – Drain Voltage Output Characteristics mA mA  The on-current of the proposed dual-gate TFT is mA while that of the conventional dual-gate TFT is mA  This result shows a 67 % enhancement in on-current mA V G = 7 V, V D = 12 V

Semiconductor & CAD Lab. Dae Yeon Lee 15  Drain Current – Drain Voltage Output Characteristics Conventional Single-gate TFT Conventional Dual-gate TFT Proposed Dual-gate TFT V G =5 V V D =10V mA0.325 mA0.508 mA V G =5 V V D =12V mA0.330 mA0.522 mA V G =7 V V D =10V mA0.508 mA0.862 mA V G =7 V V D =12V mA0.522 mA mA W/L = 2

Semiconductor & CAD Lab. Dae Yeon Lee 16  Drain Current – Drain Voltage Output Characteristics  The on-current of the proposed dual – gate TFT at different gate voltage

Semiconductor & CAD Lab. Dae Yeon Lee 17  Output Conductance Characteristics Kink starting point V G = 7 V, V D = 12 V  Reduction of the Output conductance means the reduction of the kink effect so that we can get a stable drain current in the saturation region.  The output conductance of the conventional single-gate increases about 8.3 V.

Semiconductor & CAD Lab. Dae Yeon Lee 18 Conclusion  Lowering the High electric Field at the Drain junction by Dual – Gate TFT structure  Improved Electrostatic Potential  Reduction of the Hole concentration by the holes recombine with the Floating N+ region in the channel region  On-Current is mA in the saturation region while that of the conventional dual – gate TFT is mA at V G = 7, V D = 12 V  A stable Output Conductance is accomplished by the reduction of the kink effect