Semiconductor Device Modeling and Characterization – EE5342 Lecture 10– Spring 2011 Professor Ronald L. Carter

Slides:



Advertisements
Similar presentations
Ideal Junction Theory Assumptions Ex = 0 in the chg neutral reg. (CNR)
Advertisements

EE 5340 Semiconductor Device Theory Lecture 18 – Spring 2011 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
EE 5340 Semiconductor Device Theory Lecture 12 – Spring 2011 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 14 – Spring 2011 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 8 - Fall 2009 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 11 – Spring 2011 Professor Ronald L. Carter
Semiconductor Device Modeling and Characterization – EE5342 Lecture 09– Spring 2011 Professor Ronald L. Carter
Semiconductor Device Modeling and Characterization – EE5342 Lecture 3 – Spring 2011 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 13 – Spring 2011 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 26 - Fall 2010 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 08 – Spring 2011 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 05 – Spring 2011 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 07 – Spring 2011 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 17 – Spring 2011 Professor Ronald L. Carter
L08 Feb 081 Lecture 08 Semiconductor Device Modeling and Characterization EE Spring 2001 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 15 - Fall 2009 Professor Ronald L. Carter
L23 08April031 Semiconductor Device Modeling and Characterization EE5342, Lecture 23 Spring 2003 Professor Ronald L. Carter
Semiconductor Device Modeling and Characterization – EE5342 Lecture 7 – Spring 2011 Professor Ronald L. Carter
L06 31Jan021 Semiconductor Device Modeling and Characterization EE5342, Lecture 6-Spring 2002 Professor Ronald L. Carter
Semiconductor Device Modeling and Characterization – EE5342 Lecture 5 – Spring 2011 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 15 – Spring 2011 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 27 – Spring 2011 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 19 – Spring 2011 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 24 – Spring 2011 Professor Ronald L. Carter
Semiconductor Device Modeling and Characterization – EE5342 Lecture 8 – Spring 2011 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 04 – Spring 2011 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 23 – Spring 2011 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 25 – Spring 2011 Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 10 – Fall 2010 Professor Ronald L. Carter
L04,... June 11,...1 Electronics I EE 2303/602 - Summer ‘01 Lectures 04,... Professor Ronald L. Carter
L4 January 271 Semiconductor Device Modeling and Characterization EE5342, Lecture 4-Spring 2005 Professor Ronald L. Carter
Professor Ronald L. Carter
Semiconductor Device Modeling and Characterization – EE5342 Lecture 4 – Spring 2011 Professor Ronald L. Carter
Professor Ronald L. Carter
Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 16 – Spring 2011
EE 5340 Semiconductor Device Theory Lecture 06 – Spring 2011
EE 5340 Semiconductor Device Theory Lecture 13 - Fall 2010
Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 19 – Spring 2011
Professor Ronald L. Carter
Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 05 – Spring 2011
EE 5340 Semiconductor Device Theory Lecture 04 – Spring 2011
Professor Ronald L. Carter
Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 18 – Spring 2011
EE 5340 Semiconductor Device Theory Lecture 12 – Spring 2011
Professor Ronald L. Carter
Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 26 - Fall 2009
EE 5340 Semiconductor Device Theory Lecture 14 - Fall 2009
Professor Ronald L. Carter
Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 27 - Fall 2003
Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 9 - Fall 2009
Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 15 – Spring 2011
EE 5340 Semiconductor Device Theory Lecture 07 – Spring 2011
EE 5340 Semiconductor Device Theory Lecture 13 – Spring 2011
EE 5340 Semiconductor Device Theory Lecture 29 - Fall 2010
EE 5340 Semiconductor Device Theory Lecture 17 – Spring 2011
Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 20 - Fall 2010
EE 5340 Semiconductor Device Theory Lecture 08 – Spring 2011
Professor Ronald L. Carter
EE 5340 Semiconductor Device Theory Lecture 14 - Fall 2003
Presentation transcript:

Semiconductor Device Modeling and Characterization – EE5342 Lecture 10– Spring 2011 Professor Ronald L. Carter

©rlc L10-16Feb20112 First Assignment to –In the body of the message include subscribe EE5342 This will subscribe you to the EE5342 list. Will receive all EE5342 messages If you have any questions, send to with EE5342 in subject line.

©rlc L10-16Feb20113 Second Assignment Submit a signed copy of the document that is posted at

©rlc L10-16Feb20114 Additional University Closure Means More Schedule Changes Plan to meet until noon some days in the next few weeks. This way we will make up for the lost time. The first extended class will be Monday, 2/14. The MT changed to Friday 2/18 The P1 test changed to Friday 3/11. The P2 test is still Wednesday 4/13 The Final is still Wednesday 5/11.

MT and P1 Assignment on Friday, 2/18/11 Quizzes and tests are open book –must have a legally obtained copy-no Xerox copies. –OR one handwritten page of notes. –Calculator allowed. A cover sheet will be published by Wednesday, 2/16/11. ©rlc L10-16Feb20115

6 Ideal Junction Theory Assumptions E x = 0 in the chg neutral reg. (CNR) MB statistics are applicable Neglect gen/rec in depl reg (DR) Low level injections apply so that  n p < p po for -x pc < x < -x p, and  p n < n no for x n < x < x nc Steady State conditions

©rlc L10-16Feb20117 Forward Bias Energy Bands EvEv EcEc E Fi xnxn x nc -x pc -x p 0 q(V bi -V a ) E FP E FN qV a x Imref, E Fn Imref, E Fp

©rlc L10-16Feb20118 Law of the junction (follow the min. carr.)

©rlc L10-16Feb20119 Law of the junction (cont.)

©rlc L10-16Feb Law of the junction (cont.)

©rlc L10-16Feb Injection Conditions

©rlc L10-16Feb Ideal Junction Theory (cont.) Apply the Continuity Eqn in CNR

©rlc L10-16Feb Ideal Junction Theory (cont.)

©rlc L10-16Feb Ideal Junction Theory (cont.)

©rlc L10-16Feb Excess minority carrier distr fctn

©rlc L10-16Feb Carrier Injection -x p xnxn -x pc 0 ln(carrier conc) ln N a ln N d ln n i ln n i 2 /N d ln n i 2 /N a x nc x ~V a /V t

©rlc L10-16Feb Minority carrier currents

©rlc L10-16Feb Evaluating the diode current

©rlc L10-16Feb Special cases for the diode current

©rlc L10-16Feb Ideal diode equation Assumptions: –low-level injection –Maxwell Boltzman statistics –Depletion approximation –Neglect gen/rec effects in DR –Steady-state solution only Current dens, J x = J s expd(V a /V t ) –where expd(x) = [exp(x) -1]

©rlc L10-16Feb Ideal diode equation (cont.) J s = J s,p + J s,n = hole curr + ele curr J s,p = qn i 2 D p coth(W n /L p )/(N d L p ) = qn i 2 D p /(N d W n ), W n > L p, “long” J s,n = qn i 2 D n coth(W p /L n )/(N a L n ) = qn i 2 D n /(N a W p ), W p > L n, “long” J s,n > N d

©rlc L10-16Feb Diffnt’l, one-sided diode conductance VaVa IDID Static (steady- state) diode I-V characteristic VQVQ IQIQ

©rlc L10-16Feb Diffnt’l, one-sided diode cond. (cont.)

©rlc L10-16Feb Charge distr in a (1- sided) short diode Assume N d << N a The sinh (see L12) excess minority carrier distribution becomes linear for W n << L p  p n (x n )=p n0 expd(V a /V t ) Total chg = Q’ p = Q’ p = q  p n (x n )W n /2 xnxn x x nc  p n (x n ) W n = x nc - x n Q’ p pnpn

©rlc L10-16Feb Charge distr in a 1- sided short diode Assume Quasi-static charge distributions Q’ p = Q’ p = q  p n (x n )W n /2 d  p n (x n ) = (W/2)* {  p n (x n,V a +  V) -  p n (x n,V a )} xnxn x x nc  p n (x n,V a ) Q’ p pnpn  p n (x n,V a +  V)  Q’ p

©rlc L10-16Feb Cap. of a (1-sided) short diode (cont.)

©rlc L10-16Feb General time- constant

©rlc L10-16Feb General time- constant (cont.)

©rlc L10-16Feb General time- constant (cont.)

©rlc L10-16Feb References *Fundamentals of Semiconductor Theory and Device Physics, by Shyh Wang, Prentice Hall, **Semiconductor Physics & Devices, by Donald A. Neamen, 2nd ed., Irwin, Chicago. M&K = Device Electronics for Integrated Circuits, 3rd ed., by Richard S. Muller, Theodore I. Kamins, and Mansun Chan, John Wiley and Sons, New York, Device Electronics for Integrated Circuits, 2 ed., by Muller and Kamins, Wiley, New York, Physics of Semiconductor Devices, by S. M. Sze, Wiley, New York, Physics of Semiconductor Devices, Shur, Prentice- Hall, 1990.