Velocity Saturation Effects. Ohm’s “Law” This says the Drift Velocity V d is linear in the electric field E: μ  Mobility If this were true for all E,

Slides:



Advertisements
Similar presentations
CHAPTER 4 CONDUCTION IN SEMICONDUCTORS
Advertisements

1 Carrier Action: Motion, Recombination and Generation. What happens after we figure out how many electrons and holes are in the semiconductor?
EE 5340 Semiconductor Device Theory Lecture 6 - Fall 2010 Professor Ronald L. Carter
Semiconductor Device Modeling and Characterization – EE5342 Lecture 6 – Spring 2011 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 06 – Spring 2011 Professor Ronald L. Carter
1 Fundamentals of Microelectronics  CH1 Why Microelectronics?  CH2 Basic Physics of Semiconductors  CH3 Diode Circuits  CH4 Physics of Bipolar Transistors.
Ideal Diode Equation.
Carrier Transport Phenomena
Lecture #6 OUTLINE Carrier scattering mechanisms Drift current
Lecture 2 OUTLINE Semiconductor Basics Reading: Chapter 2.
Department of Aeronautics and Astronautics NCKU Nano and MEMS Technology LAB. 1 Chapter IV June 14, 2015June 14, 2015June 14, 2015 P-n Junction.
Department of EECS University of California, Berkeley EECS 105 Fall 2003, Lecture 9 Lecture 9: PN Junctions Prof. Niknejad.
Announcements HW1 is posted, due Tuesday 9/4
EE105 Fall 2011Lecture 3, Slide 1Prof. Salahuddin, UC Berkeley Lecture 3 OUTLINE Semiconductor Basics (cont’d) – Carrier drift and diffusion PN Junction.
VLSI design Lecture 1: MOS Transistor Theory. CMOS VLSI Design3: CMOS Transistor TheorySlide 2 Outline  Introduction  MOS Capacitor  nMOS I-V Characteristics.
Spring 2007EE130 Lecture 40, Slide 1 Lecture #40 OUTLINE The MOSFET: Velocity saturation Reading: Chapter 19.1.
Lecture 3. Intrinsic Semiconductor When a bond breaks, an electron and a hole are produced: n 0 = p 0 (electron & hole concentration) Also:n 0 p 0 = n.
Ideal Diode Equation. Important Points of This Lecture There are several different techniques that can be used to determine the diode voltage and current.
Lecture 25: Semiconductors
Microscopic Ohm’s Law Outline Semiconductor Review Electron Scattering and Effective Mass Microscopic Derivation of Ohm’s Law.
Electric Current Electric current is the rate of flow of charge through some region of space The SI unit of current is the ampere (A) 1 A = 1 C / s The.
Slide # 1 SPM Probe tips CNT attached to a Si probe tip.
Electric Currents, Resistance & Electric Power
Drift and Diffusion Current
Norhayati Soin 06 KEEE 4426 WEEK 7/1 6/02/2006 CHAPTER 2 WEEK 7 CHAPTER 2 MOSFETS I-V CHARACTERISTICS CHAPTER 2.
P212c26: 1 Charge carrier motion in a conductor in two parts Constant Acceleration Randomizing Collisions (momentum, energy) =>Resulting Motion Average.
NDR & The Gunn Effect. For direct bandgap materials, like GaAs: v d vs. E peaks before saturation & decreases again, after which it finally saturates.
ECE 250 – Electronic Devices 1 ECE 250 Electronic Device Modeling.
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. ECE 255: Electronic Analysis and Design Prof. Peide (Peter)
Network for Computational Nanotechnology (NCN) UC Berkeley, Univ.of Illinois, Norfolk State, Northwestern, Purdue, UTEP First-Time User Guide Drift-Diffusion.
Lecture 4 OUTLINE Semiconductor Fundamentals (cont’d)
© 2012 Eric Pop, UIUCECE 340: Semiconductor Electronics ECE 340 Lecture 9 Temperature Dependence of Carrier Concentrations L7 and L8: how to get electron.
Current � and � Resistance Electric Current Resistance and Ohm’s Law A Model for Electrical Conduction Resistance and Temperature Superconductor Electrical.
Farzana R ZakiEEE 231: Electronics I1 Semiconductor Diode Instructor: Farzana Rahmat Zaki Senior Lecturer, EEE Eastern University.
Short Channel Effects in MOSFET
Physics Chp 19. Electric Current Movement of charge Ampere A = C/s.
High E Field Transport BW: Sect. 8.10, p 198YC, Sect. 5.4; S, Sect. 4.13; + Outside sources.
Electronics 1 Lecture 3 Moving Charge Carriers
Electron and Hole Concentrations in Extrinsic Semiconductor
Introduction to Semiconductor Technology. Outline 3 Energy Bands and Charge Carriers in Semiconductors.
Dr. Nasim Zafar Electronics 1 EEE 231 – BS Electrical Engineering Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
EE105 - Spring 2007 Microelectronic Devices and Circuits
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.
Conduction processes in semiconductors. Two form of charge carrier transport (1) Drift (due to E-field) (2) Diffusion (due to density gradient) for two.
Semiconductor Device Physics
Penn ESE370 Fall DeHon 1 ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Day 11: September 22, 2014 MOS Transistor.
Chapter 26 CURRENT ELECTRICITY Electric Current (I) –rate of positive charge passing through a surface I=dQ/dt –units Coulomb/Second = Ampere (C/s = A)
1 ME 381R Lecture 13: Semiconductors Dr. Li Shi Department of Mechanical Engineering The University of Texas at Austin Austin, TX
Semiconductor Conductivity Ch. 1, S It is well-known that in semiconductors, there are Two charge carriers! Electrons  e - & Holes  e + What is a hole?
President UniversityErwin SitompulSDP 3/1 Dr.-Ing. Erwin Sitompul President University Lecture 3 Semiconductor Device Physics
July 24,2000Gabriele Chiodini1 Measurements in magnetic field - digression Lorentz angle measurements –ATLAS measurements – CMS measurements Radiation.
Carrier Motion - Electric Fields ECE Movement of Electrons and Holes Nearly free electrons can easily move in a semiconductor since they are not.
PHYSICAL ELECTRONICS ECX 5239 PRESENTATION 01 PRESENTATION 01 Name : A.T.U.N Senevirathna. Reg, No : Center : Kandy.
Conductivity, Energy Bands and Charge Carriers in Semiconductors
ECE 333 Linear Electronics
Lecture 4 OUTLINE Semiconductor Fundamentals (cont’d)
“Low Field”  Ohm’s “Law” holds J  σE or vd  μE
Lecture 22 OUTLINE The MOSFET (cont’d) MOSFET scaling
Intro to Semiconductors and p-n junction devices
Announcements HW1 is posted, due Tuesday 9/4
Lecture 22 OUTLINE The MOSFET (cont’d) Velocity saturation
Lecture #6 OUTLINE Carrier scattering mechanisms Drift current
Lecture 4 OUTLINE Semiconductor Fundamentals (cont’d)
AP Physics L07_current Effects of moving charges
Effects of moving charges
Lecture 22 OUTLINE The MOSFET (cont’d) MOSFET scaling
Lecture 22 OUTLINE The MOSFET (cont’d) Velocity saturation
Semiconductor Physics
MOSCAP Non-idealities
Presentation transcript:

Velocity Saturation Effects

Ohm’s “Law” This says the Drift Velocity V d is linear in the electric field E: μ  Mobility If this were true for all E, the charge carriers could be made to go fast without limit, just by increasing E! That would be nonsense! So, in every material, at high enough E, the V d vs E curve must saturate to a constant value!

Ohm’s “Law” Obviously, this says that the V d vs E curve looks qualitatively like: E

Measurement shows that, in all materials, at high enough E, the V d vs E curve looks qualitatively like: E Electrons Holes

E Field Dependence of Drift the Velocity The carrier velocity saturation at high E fields clearly places a FUNDAMENTAL upper limit on the speed of semiconductor devices. Velocity Saturation In n-type Si, the saturation velocity V s ~ 10 7 cm/s at a field E s ~ 10 4 V/cm In GaAs there is a velocity reduction (peak) before saturation. We’ll discuss this later

A Simple Empirical Model for Velocity Saturation sat vdvd E E E +  1  E << E sat, V d = μE E << E sat, V d  constant Or V d  μ(E)E Where μ(E)  “Field Dependent Mobility”

A Slightly Better Model for Velocity Saturation E << E sat, V d = μE E << E sat, V d  constant

Still Another Model for Velocity Saturation: The Two Region Model

Velocity Saturation in Si Measurements show that, at E  10 4 V/cm, the carrier velocity for electrons saturates to v sat  10 7 cm/s & for holes, it saturates to v sat  8  10 6 cm/s.

Velocity Saturation in Si To model the data, use Measurements show that, at E  10 4 V/cm, the carrier velocity for electrons saturates to v sat  10 7 cm/s & for holes, it saturates to v sat  8  10 6 cm/s.

Velocity Saturation in Si To model the data, use Measurements show that, at E  10 4 V/cm, the carrier velocity for electrons saturates to v sat  10 7 cm/s & for holes, it saturates to v sat  8  10 6 cm/s. Results

Temperature Dependence of Velocity Saturation in Si Measurements: Both v sat & E are temperature dependent! Electrons

Temperature Dependence of Velocity Saturation in Si Holes

Voltage-Current Behavior in Velocity Saturation Conditions For short channel devices As expected, in the linear, Ohm’s Law Region: I = V/R In the non-linear Velocity Saturation Region, the I vs V curve bends over & saturates: I = V sat /R = I sat

Qualitative I-V Curves in Velocity Saturation Conditions Long Channel Devices Short Channel Devices I V I = V/R V ssat V lsat

I-V Curves in Velocity Saturation Conditions