CS 152 Computer Architecture and Engineering
|
|
- Myra Wade
- 6 years ago
- Views:
Transcription
1 CS 152 Computr Architctur and Enginring Lctur 11 VLSI I John Lazzaro ( TAs: Td Hong and David Marquardt www-inst.cs.brkly.du/~cs152/
2 Last Tim: Piplin Hazard Rsolution ADD R4,R3,R2 OR R2,R3,R1 AND R2,R2,R1 Which do w forward from? ID (Dcod) EX IR IR IR MEM IR WE, MmToRg WB Mux,Logic rs1 rs2 ws wd RgFil WE rd1 rd2 From WB A M op A L U 32 Y M Data Mmory Addr Dout Din WE MmToRg R Ext B
3 Today: Stat Storag Tools on Silicon ICs Capacitanc: Holds stat as charg Transistors: How to mov charg Layout: How to fabricat your IC VLSI == Vry Larg Scal Intgration Th tall thin dsignr, with ft on th ground and had in th sky. Th ground: Physics and IC Fabrication Th sky: Architctur and Applications Carvr Mad
4 Capacitanc
5 Rcall: Building a capacitor Dilctric Top Plat Conducts lctricity wll. (mtal, dopd polysilicon) An insulator. Dos not conducts lctricity at all. (air, glass (silicon dioxid)) Bottom Plat Conducts lctricity wll (mtal, dopd polysilicon)
6 Rcall: Capacitors in action Bcaus th dilctric is an insulator, and dos not conduct. I = Aftr circuit sttls... Q = C V = C * 1.5 Volts (D cll) Q: Charg stord on capacitor C: Th capacitanc of th dvic: function of dvic shap and typ of dilctric. Aftr battry is rmovd: Still, Q = C * 1.5 Volts Capacitor rmmbrs charg 1.5V
7 Capacitors and currnt... Q = C V I V Diffrntiat with rspct to tim... if C!= C(t)... dq/dt = C dv/dt I is dfind as dq/dt... I = C dv/dt Obsrvation: If a voltag chang dv occurs in zro tim (dt = 0), th currnt I is infinit (impossibl). Th voltag across a capacitor cannot chang instantanously. And by Q = C V, th charg stord on a capacitor cannot chang instantanously.
8 Storing computational stat as charg Stat is codd as th amount of nrgy stord by a dvic V Stat is rad by snsing th amount of nrgy Problms: nois changs Q (up or down), parasitics lak or sourc Q. Fortunatly, Q cannot chang instantanously, but that only gts us in th ballpark.
9 How do w fight nois and win? Stor mor nrgy than w xpct from th nois. Q = CV. To stor mor charg, us a biggr V or mak a biggr C. Cost: Powr, chip siz. Exampl: 1 bit pr capacitor. Writ 1.5 volts on C. To rad C, masur V. V > 0.75 volts is a 1. V < 0.75 volts is a 0. Cost: Could hav stord many bits on that capacitor. Rprsnt stat as charg in ways that ar robust to nois. Corrct small stat rrors that ar introducd by nois. Cost: Complxity. Ex: rad C vry 1 ms Is V > 0.75 volts? Writ back 1.5V (ys) or 0V (no).
10 MOS Transistors Two diods and a capacitor in an intrsting arrangmnt. So, w bgin with a diod rviw...
11 Diods in action... Rsistor Light mitting diod (LED) Light on? Ys! Light on? No!
12 Diods: Currnt vs Voltag Anod + Diod is off I - Io Diod is on I Io xp(v/vo) I V - Cathod I = Io [xp(v/vo) - 1] Io rang: 1fA to 1nA Vo rang: 25mV to 60 mv
13 Making a diod on a silicon wafr
14 A pur ( intrinsic ) silicon crystal... Conducts lctricity bttr than an insulator, wors than a conductor. Why? Most lctrons (dots) ar in a full valnc band. Moving in th band is difficult. Espcially nar 0 dgrs K. Lots of room, but fw lctrons. Forbiddn band gap Conduction band Valnc band Many lctrons, but packd too tight to mov. l c t r o n n r g y
15 Intrinsic silicon crystal as T riss... Som valnc band lctrons diffus into th conduction band. Ths lctrons lav bhind hols in th valnc band, allowing rmaining lctrons to mov asir. Mor lctrons, bttr conduction Conduction band Valnc band W think of hols as positiv carrirs... l c t r o n n r g y
16 W nginr crystal with impuritis...
17 N-typ silicon: add donor atoms Us diffusion or ion implantation to rplac som of th Si atoms with As Arsnsic has an xtra lctron that is donats to th conduction band. n+ : havy doping. n- : light doping. Elctrons from donor atoms. Improvs conductivy. No chang in th numbr of hols Conduction band Donor nrgy Valnc band l c t r o n n r g y
18 P-typ silicon: add accptor atoms Us diffusion or ion implantation to rplac som of th Si atoms with Boron Boron has on fwr lctron than Si. It can accpt valnc band lctrons, crating hols. p+ : havy doping. p- : light doping. No chang in conduction band lctron count Conduction band Accptor nrgy Valnc band Numbr of hols incrasd, conductivity improvs l c t r o n n r g y
19 How to mak a silicon diod V Cathod: - Anod: + n+ p- Wafr cross-sction Wafr dopd p-typ p- rgion dpltion At V = 0, hill too high for rgion lctrons to diffus up. n+ rgion For hols, going downhill is hard. no carrirs V controls hill. dpltion rgion l c t r o n n r g y
20 Diods: Currnt vs Voltag Anod + Diod is off I - Io Diod is on I Io xp(v/vo) I V - Cathod I = Io [xp(v/vo) - 1] Io rang: 1fA to 1nA Vo rang: 25mV to 60 mv
21 Not: Diods ar biasd off! V1 V2 V1 n+ n+ V2 p- 0 V - ground V1, V2 > 0V. Diods off, only currnt is Io lakag. I = Io [xp(v/vo) - 1] Anods of all diods on wafr connctd to ground.
22 Admin: Tsting and Intrfacs on Friday Homwork 1: du Friday 3/4 Midtrm 1: Thurs 3/17, 6PM to 9PM
23 MOS Transistors Two diods and a capacitor in an intrsting arrangmnt...
24 What w want: th prfct switch. V1 n+ V1 Switch is off. V1 is not connctd to V2. p- Switch is on. V1 is connctd to V2. n+ p- V2 n+ V2 W want to turn a p-typ rgion into an n-typ rgion undr voltag control. W nd lctrons to fill valnc hols and add conduction band lctrons
25 An n-channl MOS transistor (nfet) Vd = 1V Vd = 1V I na n+ I µa n+ Vg = 0V dilctric p- Vg = 1V dilctric p- n+ Vs = 0V n+ Vs = 0V Polysilicon gat, dilctric, and substrat form a capacitor. nft is off (I is lakag ) Vg = 1V, small rgion nar th surfac turns from p-typ to n-typ. nft is on.
26 Drawing an nfet Mask drawings snt to th fabrication facility to mak th chips.
27 Mask st for an n-ft (circa 1986) Vg = 0V Vd = 1V I na n+ dilctric p- Vs = 0V Masks #1: n+ diffusion n+ #2: poly (gat) #3: diff contact #4: mtal Top-down viw: Layrs to do p-ft not shown. Modrn procsss hav mor 6 to 10 mtal layrs (in 1986: 2)
28 Dsign ruls for masks, Poly ovrhang. So that if masks ar misalignd, w still gt --- in channl. Minimum gat lngth. So that th sourc and drain dpltion rgions do not mt! lngth Mtal ruls: Contact sparation from channl, on fixd contact siz, ovrlap ruls with mtal, tc... #1: n+ diffusion #3: diff contact #2: poly (gat) #4: mtal
29 Lssons larnd Capacitors hold stat Smiconductor physics Drawing transistors
30 Lcturs: Coming up nxt... Transistor quations, basic mmory circuits. Mmory array structurs and intrfacs. Th mmory hirarchy
CS 152 Computer Architecture and Engineering. Lecture 11 VLSI
CS 152 Computer Architecture and Engineering Lecture 11 VLSI 2005-10-6 John Lazzaro (www.cs.berkeley.edu/~lazzaro) TAs: David Marquardt and Udam Saini www-inst.eecs.berkeley.edu/~cs152/ Today: State Storage
More informationCS 152 Computer Architecture and Engineering
CS 152 Computer Architecture and Engineering Lecture 12 VLSI II 2005-2-24 John Lazzaro (www.cs.berkeley.edu/~lazzaro) TAs: Ted Hong and David Marquardt www-inst.eecs.berkeley.edu/~cs152/ Last Time: Device
More informationThe pn junction: 2 Current vs Voltage (IV) characteristics
Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n
More informationSolid State Device Fundamentals
Solid Stat vic Fundamntal ES 345 Lctur Cour by landr M. Zaitv alandr.zaitv@ci.cuny.du Tl: 718 98 81 4101b Collg of Statn Iland / CUY p-n Junction p-n junction i a phyical contact of p- and n-typ miconductor.
More informationExam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.
Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r
More informationVoltage, Current, Power, Series Resistance, Parallel Resistance, and Diodes
Lctur 1. oltag, Currnt, Powr, Sris sistanc, Paralll sistanc, and Diods Whn you start to dal with lctronics thr ar thr main concpts to start with: Nam Symbol Unit oltag volt Currnt ampr Powr W watt oltag
More informationLast time. Resistors. Circuits. Question. Quick Quiz. Quick Quiz. ( V c. Which bulb is brighter? A. A B. B. C. Both the same
Last tim Bgin circuits Rsistors Circuits Today Rsistor circuits Start rsistor-capacitor circuits Physical layout Schmatic layout Tu. Oct. 13, 2009 Physics 208 Lctur 12 1 Tu. Oct. 13, 2009 Physics 208 Lctur
More informationExam 2 Thursday (7:30-9pm) It will cover material through HW 7, but no material that was on the 1 st exam.
Exam 2 Thursday (7:30-9pm) It will covr matrial through HW 7, but no matrial that was on th 1 st xam. What happns if w bash atoms with lctrons? In atomic discharg lamps, lots of lctrons ar givn kintic
More informationMath 34A. Final Review
Math A Final Rviw 1) Us th graph of y10 to find approimat valus: a) 50 0. b) y (0.65) solution for part a) first writ an quation: 50 0. now tak th logarithm of both sids: log() log(50 0. ) pand th right
More informationLecture 18 - Semiconductors - continued
Lctur 18 - Smiconductors - continud Lctur 18: Smiconductors - continud (Kittl C. 8) + a - Donors and accptors Outlin Mor on concntrations of lctrons and ols in Smiconductors Control of conductivity by
More informationElectrochemistry L E O
Rmmbr from CHM151 A rdox raction in on in which lctrons ar transfrrd lctrochmistry L O Rduction os lctrons xidation G R ain lctrons duction W can dtrmin which lmnt is oxidizd or rducd by assigning oxidation
More informationSolid State Theory Physics 545 Band Theory III
Solid Stat Thory Physics 545 Band Thory III ach atomic orbital lads to a band of allowd stats in th solid Band of allowd stats Gap: no allowd stats Band of allowd stats Gap: no allowd stats Band of allowd
More informationPart 7: Capacitance And Capacitors
Part 7: apacitanc And apacitors 7. Elctric harg And Elctric Filds onsidr a pair of flat, conducting plats, arrangd paralll to ach othr (as in figur 7.) and sparatd by an insulator, which may simply b air.
More informationQuantitative Model of Unilluminated Diode part II. G.R. Tynan UC San Diego MAE 119 Lecture Notes
Quantitativ Modl of Unilluminatd Diod part II G.R. Tynan UC San Digo MAE 119 Lctur Nots Minority Carrir Dnsity at dg of quasinutral rgion incrass EXPONENTIALLY forward bias p nb n pa = p n0 xp qv a kt
More informationElectromagnetism Physics 15b
lctromagntism Physics 15b Lctur #8 lctric Currnts Purcll 4.1 4.3 Today s Goals Dfin lctric currnt I Rat of lctric charg flow Also dfin lctric currnt dnsity J Charg consrvation in a formula Ohm s Law vryon
More informationChapter 2 The Well 9/5/2017. E E 480 Introduction to Analog and Digital VLSI Paul M. Furth New Mexico State University
hapter 2 The Well E E 480 Introduction to Analog and Digital VLSI Paul M. Furth New Mexico State University p+ sub ~ 150 m thick, p-epi ~ 30 m thick All transistors go in p- epi layer Typical p- doping
More informationLecture 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 informationStatus of LAr TPC R&D (2) 2014/Dec./23 Neutrino frontier workshop 2014 Ryosuke Sasaki (Iwate U.)
Status of LAr TPC R&D (2) 214/Dc./23 Nutrino frontir workshop 214 Ryosuk Sasaki (Iwat U.) Tabl of Contnts Dvlopmnt of gnrating lctric fild in LAr TPC Introduction - Gnrating strong lctric fild is on of
More informationChapter 6 Folding. Folding
Chaptr 6 Folding Wintr 1 Mokhtar Abolaz Folding Th folding transformation is usd to systmatically dtrmin th control circuits in DSP architctur whr multipl algorithm oprations ar tim-multiplxd to a singl
More informationESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems. Today MOS MOS. Capacitor. Idea
ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Day 9: September 26, 2011 MOS Model Today MOS Structure Basic Idea Semiconductor Physics Metals, insulators Silicon lattice
More informationMOS Transistor I-V Characteristics and Parasitics
ECEN454 Digital Integrated Circuit Design MOS Transistor I-V Characteristics and Parasitics ECEN 454 Facts about Transistors So far, we have treated transistors as ideal switches An ON transistor passes
More informationDavisson Germer experiment Announcements:
Davisson Grmr xprimnt Announcmnts: Homwork st 7 is du Wdnsday. Problm solving sssions M3-5, T3-5. Th 2 nd midtrm will b April 7 in MUEN E0046 at 7:30pm. BFFs: Davisson and Grmr. Today w will go ovr th
More informationE hf. hf c. 2 2 h 2 2 m v f ' f 2f ' f cos c
EXPERIMENT 9: COMPTON EFFECT Rlatd Topics Intractions of photons with lctrons, consrvation of momntum and nrgy, inlastic and lastic scattring, intraction cross sction, Compton wavlngth. Principl Whn photons
More informationLecture Outline. Skin Depth Power Flow 8/7/2018. EE 4347 Applied Electromagnetics. Topic 3e
8/7/018 Cours Instructor Dr. Raymond C. Rumpf Offic: A 337 Phon: (915) 747 6958 E Mail: rcrumpf@utp.du EE 4347 Applid Elctromagntics Topic 3 Skin Dpth & Powr Flow Skin Dpth Ths & Powr nots Flow may contain
More informationGradebook & Midterm & Office Hours
Your commnts So what do w do whn on of th r's is 0 in th quation GmM(1/r-1/r)? Do w nd to driv all of ths potntial nrgy formulas? I don't undrstand springs This was th first lctur I actually larnd somthing
More informationESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems
ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Lec 6: September 18, 2017 MOS Model You are Here: Transistor Edition! Previously: simple models (0 and 1 st order) " Comfortable
More informationFundamentals of the Metal Oxide Semiconductor Field-Effect Transistor
Triode Working FET Fundamentals of the Metal Oxide Semiconductor Field-Effect Transistor The characteristics of energy bands as a function of applied voltage. Surface inversion. The expression for the
More informationESE 570: Digital Integrated Circuits and VLSI Fundamentals
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 4: January 29, 2019 MOS Transistor Theory, MOS Model Penn ESE 570 Spring 2019 Khanna Lecture Outline! CMOS Process Enhancements! Semiconductor
More information6.1 Integration by Parts and Present Value. Copyright Cengage Learning. All rights reserved.
6.1 Intgration by Parts and Prsnt Valu Copyright Cngag Larning. All rights rsrvd. Warm-Up: Find f () 1. F() = ln(+1). F() = 3 3. F() =. F() = ln ( 1) 5. F() = 6. F() = - Objctivs, Day #1 Studnts will b
More informationSection 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 informationELEN0037 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 informationElectrochemical Energy Systems Spring 2014 MIT, M. Z. Bazant. Midterm Exam
10.66 Elctrochmical Enrgy Systms Spring 014 MIT, M. Z. Bazant Midtrm Exam Instructions. This is a tak-hom, opn-book xam du in Lctur. Lat xams will not b accptd. You may consult any books, handouts, or
More informationu r du = ur+1 r + 1 du = ln u + C u sin u du = cos u + C cos u du = sin u + C sec u tan u du = sec u + C e u du = e u + C
Tchniqus of Intgration c Donald Kridr and Dwight Lahr In this sction w ar going to introduc th first approachs to valuating an indfinit intgral whos intgrand dos not hav an immdiat antidrivativ. W bgin
More informationEEO 401 Digital Signal Processing Prof. Mark Fowler
EEO 401 Digital Signal Procssing Prof. Mark Fowlr ot St #18 Introduction to DFT (via th DTFT) Rading Assignmnt: Sct. 7.1 of Proakis & Manolakis 1/24 Discrt Fourir Transform (DFT) W v sn that th DTFT is
More informationESE 570: Digital Integrated Circuits and VLSI Fundamentals
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 4: January 23, 2018 MOS Transistor Theory, MOS Model Penn ESE 570 Spring 2018 Khanna Lecture Outline! CMOS Process Enhancements! Semiconductor
More informationIntroduction to CMOS VLSI Design Lecture 1: Introduction
Introduction to CMOS VLSI Design Lecture 1: Introduction David Harris, Harvey Mudd College Kartik Mohanram and Steven Levitan University of Pittsburgh Introduction Integrated circuits: many transistors
More informationEECE 301 Signals & Systems Prof. Mark Fowler
EECE 301 Signals & Systms Prof. Mark Fowlr ot St #21 D-T Signals: Rlation btwn DFT, DTFT, & CTFT 1/16 W can us th DFT to implmnt numrical FT procssing This nabls us to numrically analyz a signal to find
More informationLecture 3: CMOS Transistor Theory
Lecture 3: CMOS Transistor Theory Outline Introduction MOS Capacitor nmos I-V Characteristics pmos I-V Characteristics Gate and Diffusion Capacitance 2 Introduction So far, we have treated transistors
More informationEE 5211 Analog Integrated Circuit Design. Hua Tang Fall 2012
EE 5211 Analog Integrated Circuit Design Hua Tang Fall 2012 Today s topic: 1. Introduction to Analog IC 2. IC Manufacturing (Chapter 2) Introduction What is Integrated Circuit (IC) vs discrete circuits?
More informationPHYS ,Fall 05, Term Exam #1, Oct., 12, 2005
PHYS1444-,Fall 5, Trm Exam #1, Oct., 1, 5 Nam: Kys 1. circular ring of charg of raius an a total charg Q lis in th x-y plan with its cntr at th origin. small positiv tst charg q is plac at th origin. What
More informationPH2200 Practice Final Exam Spring 2004
PH2200 Practic Final Exam Spring 2004 Instructions 1. Writ your nam and studnt idntification numbr on th answr sht. 2. This a two-hour xam. 3. Plas covr your answr sht at all tims. 4. This is a closd book
More informationThe following information relates to Questions 1 to 4:
Th following information rlats to Qustions 1 to 4: QUESTIN 1 Th lctrolyt usd in this ful cll is D watr carbonat ions hydrogn ions hydroxid ions QUESTIN 2 Th product formd in th ful cll is D hydrogn gas
More informationPair (and Triplet) Production Effect:
Pair (and riplt Production Effct: In both Pair and riplt production, a positron (anti-lctron and an lctron (or ngatron ar producd spontanously as a photon intracts with a strong lctric fild from ithr a
More informationLecture #15. Bipolar Junction Transistors (BJTs)
ctur #5 OUTN Th iolar Junction Transistor Fundamntals dal Transistor Analysis Rading: hatr 0,. 30 ctur 5, Slid iolar Junction Transistors (JTs Ovr th ast 3 ads, th highr layout dnsity and low-owr advantag
More informationQuantum manipulation and qubits
Quantum manipulation and qubits Qubits Quantum information Quantum tlportation Rsonant manipulation Diabatic and adiabatic manipulation Quantum gats Quantiation of a osphson junction Phas qubit Coulomb
More informationMOSFET: 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 informationGeneral Notes About 2007 AP Physics Scoring Guidelines
AP PHYSICS C: ELECTRICITY AND MAGNETISM 2007 SCORING GUIDELINES Gnral Nots About 2007 AP Physics Scoring Guidlins 1. Th solutions contain th most common mthod of solving th fr-rspons qustions and th allocation
More informationGive the letter that represents an atom (6) (b) Atoms of A and D combine to form a compound containing covalent bonds.
1 Th diagram shows th lctronic configurations of six diffrnt atoms. A B C D E F (a) You may us th Priodic Tabl on pag 2 to hlp you answr this qustion. Answr ach part by writing on of th lttrs A, B, C,
More information! Previously: simple models (0 and 1 st order) " Comfortable with basic functions and circuits. ! This week and next (4 lectures)
ESE370: CircuitLevel Modeling, Design, and Optimization for Digital Systems Lec 6: September 18, 2017 MOS Model You are Here: Transistor Edition! Previously: simple models (0 and 1 st order) " Comfortable
More informationElectronics Fets and Mosfets Prof D C Dube Department of Physics Indian Institute of Technology, Delhi
Electronics Fets and Mosfets Prof D C Dube Department of Physics Indian Institute of Technology, Delhi Module No. #05 Lecture No. #02 FETS and MOSFETS (contd.) In the previous lecture, we studied the working
More informationCh. 24 Molecular Reaction Dynamics 1. Collision Theory
Ch. 4 Molcular Raction Dynamics 1. Collision Thory Lctur 16. Diffusion-Controlld Raction 3. Th Matrial Balanc Equation 4. Transition Stat Thory: Th Eyring Equation 5. Transition Stat Thory: Thrmodynamic
More informationOn the Hamiltonian of a Multi-Electron Atom
On th Hamiltonian of a Multi-Elctron Atom Austn Gronr Drxl Univrsity Philadlphia, PA Octobr 29, 2010 1 Introduction In this papr, w will xhibit th procss of achiving th Hamiltonian for an lctron gas. Making
More information! CMOS Process Enhancements. ! Semiconductor Physics. " Band gaps. " Field Effects. ! MOS Physics. " Cut-off. " Depletion.
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 4: January 9, 019 MOS Transistor Theory, MOS Model Lecture Outline CMOS Process Enhancements Semiconductor Physics Band gaps Field Effects
More information7.4 Potential Difference and Electric Potential
7.4 Potntial Diffrnc and Elctric Potntial In th prvious sction, you larnd how two paralll chargd surfacs produc a uniform lctric fild. From th dfinition of an lctric fild as a forc acting on a charg, it
More informationLecture 34: Portable Systems Technology Background Professor Randy H. Katz Computer Science 252 Fall 1995
Lecture 34: Portable Systems Technology Background Professor Randy H. Katz Computer Science 252 Fall 1995 RHK.F95 1 Technology Trends: Microprocessor Capacity 100000000 10000000 Pentium Transistors 1000000
More informationLecture 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 informationIXBT22N300HV IXBH22N300HV
High Voltag, High Gain BIMOSFT TM Monolithic Bipolar MOS Transistor Advanc Tchnical Information IXBTNHV IXBHNHV V CS = V = A V C(sat). TO-6HV (IXBT) Symbol Tst Conditions Maximum Ratings V CS = 5 C to
More informationCMPEN 411 VLSI Digital Circuits. Lecture 03: MOS Transistor
CMPEN 411 VLSI Digital Circuits Lecture 03: MOS Transistor Kyusun Choi [Adapted from Rabaey s Digital Integrated Circuits, Second Edition, 2003 J. Rabaey, A. Chandrakasan, B. Nikolic] CMPEN 411 L03 S.1
More informationESE370: 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 informationSeptember 23, Honors Chem Atomic structure.notebook. Atomic Structure
Atomic Structur Topics covrd Atomic structur Subatomic particls Atomic numbr Mass numbr Charg Cations Anions Isotops Avrag atomic mass Practic qustions atomic structur Sp 27 8:16 PM 1 Powr Standards/ Larning
More informationFourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation.
Lur 7 Fourir Transforms and th Wav Euation Ovrviw and Motivation: W first discuss a fw faturs of th Fourir transform (FT), and thn w solv th initial-valu problm for th wav uation using th Fourir transform
More informationLecture 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 informationThe Intrinsic Silicon
The Intrinsic ilicon Thermally generated electrons and holes Carrier concentration p i =n i ni=1.45x10 10 cm-3 @ room temp Generally: n i = 3.1X10 16 T 3/2 e -1.21/2KT cm -3 T= temperature in K o (egrees
More informationElements of Statistical Thermodynamics
24 Elmnts of Statistical Thrmodynamics Statistical thrmodynamics is a branch of knowldg that has its own postulats and tchniqus. W do not attmpt to giv hr vn an introduction to th fild. In this chaptr,
More informationDifferential Equations
Prfac Hr ar m onlin nots for m diffrntial quations cours that I tach hr at Lamar Univrsit. Dspit th fact that ths ar m class nots, th should b accssibl to anon wanting to larn how to solv diffrntial quations
More informationECE 344 Microwave Fundamentals
ECE 44 Microwav Fundamntals Lctur 08: Powr Dividrs and Couplrs Part Prpard By Dr. hrif Hkal 4/0/08 Microwav Dvics 4/0/08 Microwav Dvics 4/0/08 Powr Dividrs and Couplrs Powr dividrs, combinrs and dirctional
More informationλ = 2L n Electronic structure of metals = 3 = 2a Free electron model Many metals have an unpaired s-electron that is largely free
5.6 4 Lctur #4-6 pag Elctronic structur of mtals r lctron modl Many mtals av an unpaird s-lctron tat is largly fr Simplst modl: Particl in a box! or a cubic box of lngt L, ψ ( xyz) 8 xπ ny L L L n x π
More informationEE 330 Lecture 12. Devices in Semiconductor Processes. Resistors Diodes
EE 330 Lecture 12 evices in Semiconductor Processes Resistors iodes Exam 1 Friday Feb 16 Students may bring 1 page of notes HW assignment of week of Feb 11 due on Wed Sfeb 14 at beginning of class No 5:00
More informationLecture 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 informationJunction Diodes. Tim Sumner, Imperial College, Rm: 1009, x /18/2006
Junction Diodes Most elementary solid state junction electronic devices. They conduct in one direction (almost correct). Useful when one converts from AC to DC (rectifier). But today diodes have a wide
More informationECE 497 JS Lecture - 12 Device Technologies
ECE 497 JS Lecture - 12 Device Technologies Spring 2004 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jose@emlab.uiuc.edu 1 NMOS Transistor 2 ρ Source channel charge density
More information4 x 4, and. where x is Town Square
Accumulation and Population Dnsity E. A city locatd along a straight highway has a population whos dnsity can b approimatd by th function p 5 4 th distanc from th town squar, masurd in mils, whr 4 4, and
More informationLECTURE 23. MOS transistor. 1 We need a smart switch, i.e., an electronically controlled switch. Lecture Digital Circuits, Logic
LECTURE 23 Lecture 16-20 Digital Circuits, Logic 1 We need a smart switch, i.e., an electronically controlled switch 2 We need a gain element for example, to make comparators. The device of our dreams
More informationMOS transistors (in subthreshold)
MOS tanito (in ubthhold) Hitoy o th Tanito Th tm tanito i a gnic nam o a olid-tat dvic with 3 o mo tminal. Th ild-ct tanito tuctu wa it dcibd in a patnt by J. Lilinld in th 193! t took about 4 ya bo MOS
More informationDifferentiation of Exponential Functions
Calculus Modul C Diffrntiation of Eponntial Functions Copyright This publication Th Northrn Albrta Institut of Tchnology 007. All Rights Rsrvd. LAST REVISED March, 009 Introduction to Diffrntiation of
More informationCMOS Digital Integrated Circuits Lec 13 Semiconductor Memories
Lec 13 Semiconductor Memories 1 Semiconductor Memory Types Semiconductor Memories Read/Write (R/W) Memory or Random Access Memory (RAM) Read-Only Memory (ROM) Dynamic RAM (DRAM) Static RAM (SRAM) 1. Mask
More informationAnalytical Modelling of conventional DMG-SOI MOSFET using Different Gate Dielectric Material
Intrnational Journal of Enginring Tchnology, Managmnt and Applid Scincs www.ijtmas.com May 017, olum 5, Issu 5, ISSN 349-4476 Analytical Modlling of convntional DMG-SOI MOSFET using Diffrnt Gat Dilctric
More informationVLSI Design I; A. Milenkovic 1
Review: implified CMO Inverter Process CPE/EE 7, CPE 7 VLI esign I L: MO Transistor cut line epartment of Electrical and Computer Engineering University of Alabama in Huntsville Aleksandar Milenkovic (
More informationY 0. Standing Wave Interference between the incident & reflected waves Standing wave. A string with one end fixed on a wall
Staning Wav Intrfrnc btwn th incint & rflct wavs Staning wav A string with on n fix on a wall Incint: y, t) Y cos( t ) 1( Y 1 ( ) Y (St th incint wav s phas to b, i.., Y + ral & positiv.) Rflct: y, t)
More informationA central nucleus. Protons have a positive charge Electrons have a negative charge
Atomic Structur Lss than ninty yars ago scintists blivd that atoms wr tiny solid sphrs lik minut snookr balls. Sinc thn it has bn discovrd that atoms ar not compltly solid but hav innr and outr parts.
More informationDerivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian
Drivation of Elctron-Elctron Intraction Trms in th Multi-Elctron Hamiltonian Erica Smith Octobr 1, 010 1 Introduction Th Hamiltonian for a multi-lctron atom with n lctrons is drivd by Itoh (1965) by accounting
More information! CMOS Process Enhancements. ! Semiconductor Physics. " Band gaps. " Field Effects. ! MOS Physics. " Cut-off. " Depletion.
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 4: January 3, 018 MOS Transistor Theory, MOS Model Lecture Outline! CMOS Process Enhancements! Semiconductor Physics " Band gaps " Field Effects!
More informationSurface Mount RF Schottky Barrier Diodes. Technical Data. GUx. HSMS-281x Series
Surface Mount RF Schottky Barrier Diodes Technical Data HSMS-28x Series Features Surface Mount Packages Low Flicker Noise Low FIT (Failure in Time) Rate* Six-sigma Quality Level Single, Dual and Quad Versions
More informationClass 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 informationChapter 3 Basics Semiconductor Devices and Processing
Chapter 3 Basics Semiconductor Devices and Processing Hong Xiao, Ph. D. www2.austin.cc.tx.us/hongxiao/book.htm Hong Xiao, Ph. D. www2.austin.cc.tx.us/hongxiao/book.htm 1 Objectives Identify at least two
More informationDigital Integrated Circuits A Design Perspective
Semiconductor Memories Adapted from Chapter 12 of Digital Integrated Circuits A Design Perspective Jan M. Rabaey et al. Copyright 2003 Prentice Hall/Pearson Outline Memory Classification Memory Architectures
More informationPhysics 312 First Pledged Problem Set
Physics 31 First Pldgd Problm St 1. Th ground stat of hydrogn is dscribd by th wavfunction whr a is th Bohr radius. (a) Comput th charg dnsity à (r) = 1 p ¼ µ 1 a 3 r=a ; ½ (r) = jã (r)j : and plot 4¼r
More informationESE 570: Digital Integrated Circuits and VLSI Fundamentals
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 4: January 24, 2017 MOS Transistor Theory, MOS Model Penn ESE 570 Spring 2017 Khanna Lecture Outline! Semiconductor Physics " Band gaps "
More informationHow can I control light? (and rule the world?)
How can I control light? (and rul th world?) "You know, I hav on simpl rqust. And that is to hav sharks with frickin' lasr bams attachd to thir hads! - Dr. Evil Phys 230, Day 35 Qustions? Spctra (colors
More informationSPH4U Electric Charges and Electric Fields Mr. LoRusso
SPH4U lctric Chargs an lctric Fils Mr. LoRusso lctricity is th flow of lctric charg. Th Grks first obsrv lctrical forcs whn arly scintists rubb ambr with fur. Th notic thy coul attract small bits of straw
More informationCourse Administration. CPE/EE 427, CPE 527 VLSI Design I L04: MOS Transistors. Review: CMOS Process at a Glance
Course Administration CPE/EE 7, CPE 7 VLI esign I L: MO Transistors epartment of Electrical and Computer Engineering University of Alabama in Huntsville Aleksandar Milenkovic ( www.ece.uah.edu/~milenka
More informationModel neurons!!the membrane equation!
Modl nurons!!th bran quation! Suggstd rading:! Chaptr 5.1-5.3 in Dayan, P. & Abbott, L., Thortical Nuroscinc, MIT Prss, 2001.! Modl nurons: Th bran quation! Contnts:!!!!!! Ion channls Nnst quation Goldan-Hodgkin-Katz
More informationMOS Transistor Properties Review
MOS Transistor Properties Review 1 VLSI Chip Manufacturing Process Photolithography: transfer of mask patterns to the chip Diffusion or ion implantation: selective doping of Si substrate Oxidation: SiO
More informationLecture 6 Power Zhuo Feng. Z. Feng MTU EE4800 CMOS Digital IC Design & Analysis 2010
EE4800 CMOS Digital IC Design & Analysis Lecture 6 Power Zhuo Feng 6.1 Outline Power and Energy Dynamic Power Static Power 6.2 Power and Energy Power is drawn from a voltage source attached to the V DD
More information22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.
Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M
More informationDiodes. anode. cathode. cut-off. Can be approximated by a piecewise-linear-like characteristic. Lecture 9-1
Diodes mplest nonlinear circuit element Basic operation sets the foundation for Bipolar Junction Transistors (BJTs) Also present in Field Effect Transistors (FETs) Ideal diode characteristic anode cathode
More informationChapter 2. Design and Fabrication of VLSI Devices
Chapter 2 Design and Fabrication of VLSI Devices Jason Cong 1 Design and Fabrication of VLSI Devices Objectives: To study the materials used in fabrication of VLSI devices. To study the structure of devices
More informationOutline. Why speech processing? Speech signal processing. Advanced Multimedia Signal Processing #5:Speech Signal Processing 2 -Processing-
Outlin Advancd Multimdia Signal Procssing #5:Spch Signal Procssing -Procssing- Intllignt Elctronic Systms Group Dpt. of Elctronic Enginring, UEC Basis of Spch Procssing Nois Rmoval Spctral Subtraction
More informationQuiz #1 Practice Problem Set
Name: Student Number: ELEC 3908 Physical Electronics Quiz #1 Practice Problem Set? Minutes January 22, 2016 - No aids except a non-programmable calculator - All questions must be answered - All questions
More informationSection 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