36
1 1 MOS Transistor Theory So far, we have viewed a MOS transistor as an ideal switch (digital operation) Reality: less than ideal 2 Introduction So far, we have treated transistors as ideal switches An ON transistor passes a nite amount of current Depends on terminal voltages Derive current-voltage (I-V) relationships Transistor gate, source, drain all have capacitance I = C (V/t) -> t = (C/I) V Capacitance and current determine speed

MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

  • Upload
    others

  • View
    30

  • Download
    1

Embed Size (px)

Citation preview

Page 1: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

1

1

MOS Transistor Theory

• So far, we have viewed a MOS transistor as an ideal switch (digital operation)– Reality: less than ideal

2

Introduction• So far, we have treated transistors as ideal

switches

• An ON transistor passes a finite amount of current– Depends on terminal voltages

– Derive current-voltage (I-V) relationships

• Transistor gate, source, drain all have capacitance– I = C ( V/ t) -> t = (C/I) V

– Capacitance and current determine speed

Page 2: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

2

3

MOS Capacitor• Gate and body form MOS

capacitor

• Operating modes

– Accumulation

– Depletion

– Inversion

4

MOS Transistor Theory

• Study conducting channel between source and drain• Modulated by voltage applied to the gate (voltage-controlled device)• nMOS transistor: majority carriers are electrons (greater mobility), p-substrate doped (positively doped)• pMOS transistor: majority carriers are holes (less mobility), n-substrate (negatively doped)

Page 3: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

3

5

Gate Biasing

p-substrate

n+ n+

Source Gate Drain

Channel

+ -

E

SiO2

VSS (Gnd)

• Vgs=0: no current flows from source to drain (insulated by two reverse biased pn junctions

• Vgs>0: electric field created across substrate

• Electrons accumulate under gate: region changes from p-type to n-type• Conduction path between source and drain

6

nMOS Device Behavior

Vgs << Vt

Polysilicon gatep-substrate

Accumulationmode

• Enhancement-mode transistor: Conducts when gate bias Vgs > Vt

• Depletion-mode transistor: Conducts when gate bias is zero

Vgs = Vt

Depletion mode

Depletion region

Oxide insulator

Vgs > Vt

Inversion mode

Depletion region

InversionRegion(n-type)

Page 4: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

4

EE 261 Krish Chakrabarty 7

Transistor Operating Regions

• Cut-off region: accumulation mode, zero current flow

• Linear region: Vds <= Vgs-Vt, weak inversion layer, drain current depends on Vgs and Vds

• Saturated region: Vds > Vgs-Vt, strong inversion layer, drain current independent of Vds

8

Terminal Voltages• Mode of operation depends on Vg, Vd, Vs

– Vgs = Vg – Vs

– Vgd = Vg – Vd

– Vds = Vd – Vs = Vgs - Vgd

• Source and drain are symmetric diffusion terminals

– By convention, source is terminal at lower voltage

– Hence Vds 0

• nMOS body is grounded. First assume source is 0 too.

• Three regions of operation

– Cutoff

– Linear

– Saturation

Page 5: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

5

9

nMOS Cutoff

• No channel

• Ids 0

10

nMOS Linear

• Channel forms

• Current flows from d to s – e- from s to d

• Ids increases with Vds

• Similar to linear resistor

Page 6: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

6

11

nMOS Saturation• Channel pinches off

• Ids independent of Vds

• We say current saturates

• Similar to current source

EE 261 Krish Chakrabarty 12

Threshold Voltage: Concept

Page 7: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

7

EE 261 Krish Chakrabarty 13

Current-Voltage Relations

EE 261 Krish Chakrabarty 14

Current-Voltage Relations

Page 8: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

8

EE 261 Krish Chakrabarty 15

Current-Voltage Relations

k n: transconductance of transistorW : width-to-length ratio L

• As W increases, more carriers available to conduct current

• As L increases, Vds diminishes in effect (more voltage drop). Takes longer to push carriers across the transistor, reducing current flow

EE 261 Krish Chakrabarty 16

Typical Parameter Values

k Vt

n-type 24 microA/V2 0.8Vp-type 9 microA/V2 -0.8V

Why is k higher for n-type transistors?

Page 9: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

9

EE 261 Krish Chakrabarty 17

Transistor in Saturation

Channel is pinched off

3: CMOS Transistor Theory

18

nMOS I-V Summary

• Shockley 1st order transistor models

Page 10: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

10

19

pMOS I-V

• All dopings and voltages are inverted for pMOS– Source is the more positive terminal

• Mobility μp is determined by holes– Typically 2-3x lower than that of electrons μn

– 120 cm2/V•s in AMI 0.6 μm process

• Thus pMOS must be wider to

provide same current

20

Capacitance

• Any two conductors separated by an insulator have capacitance

• Gate to channel capacitor is very important– Creates channel charge necessary for operation

• Source and drain have capacitance to body– Across reverse-biased diodes

– Called diffusion capacitance because it is associated with source/drain diffusion

Page 11: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

11

21

Gate Capacitance• Approximate channel as connected to source

• Cgs = oxWL/tox = CoxWL = CpermicronW

• Cpermicron is typically about 2 fF/μm

EE 261 Krish Chakrabarty 22

The Gate Capacitance

Page 12: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

12

23

Diffusion Capacitance

• Csb, Cdb

• Undesirable, called parasitic capacitance

• Capacitance depends on area and perimeter– Use small diffusion nodes

– Comparable to Cg

for contacted diff

– Cg for uncontacted

– Varies with process

24

Diffusion Capacitance

Page 13: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

13

25

Parasitic Resistances

W

LD

Drain

Draincontact

Polysilicon gate

DS

G

RS RD

VGS,eff

RS = (LS/W)R + RC

RD = (LD/W)R + RC

RC: contact resistance

R : sheet resistance per square of drain-source diffusion

26

Body Effect

• Many MOS devices on a common substrate– Substrate voltage of all devices are normally equal

• But several devices may be connected in series– Increase in source-to-substrate voltage as we proceed vertically

along the chain

d1

d2

s1

s2

V12

V11

g1

g2

Vsb1 = 0

Vsb2 = 0• Net effect: slight increase in threshold voltage Vt, Vt2>Vt1

Page 14: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

14

27

Making Chips

Chemicals

Wafers

Masks

ProcessingProcessed

wafer Chips

28

CMOS Fabrication

• CMOS transistors are fabricated on silicon wafer

• Lithography process similar to printing press

• On each step, different materials are deposited or etched

• Easiest to understand by viewing both top and cross-section of wafer in a simplified manufacturing process

Page 15: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

15

29

Fabrication Steps

• Features are patterned on a wafer by a photolithographic process– Photo-light lithography, n. process of printing from a plane surface

on which image to be printed is ink-receptive and the blank area is ink-repellant

• Cover the wafer with a light-sensitive, organic material called photoresist

• Expose to light with the proper pattern (mask)

• Patterns left by photoresist can be used to control where oxide is grown or materials are placed on surface of wafer

30

Basic Processing Steps

• N-diffusion created by doping regions of the substrate

• Poly and metal are laid over the substrate, with oxide to insulate them from substrate and each other

• Wires are added in layers, alternating with oxide

• Vias are cut in the oxide

Page 16: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

16

31

Basic Fabrication Steps• Layout contains information on what patterns have

to made on the wafer

• Masks are created using the layout information provided by the designer

• Procedure involves selective removal of the oxide– Coat the oxide with photoresist, polymerized by UV

light (applied through mask)

– Polymerized photoresist dissolves in acid

– Photoresist itself is acid-resistant

32

Basic Processing Steps

• Start with wafer at current step

• Add photoresist

• Pattern photoresist with mask

• Step-specific etch, implant, etc.

• Wash off resist

Page 17: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

17

Inverter Cross-section• Typically use p-type substrate for nMOS

transistors

• Requires n-well for body of pMOS transistors

34

Well and Substrate Taps• Substrate must be tied to GND and n-well to VDD

• Metal to lightly-doped semiconductor forms poor connection called Shottky Diode

• Use heavily doped well and substrate contacts / taps

Page 18: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

18

Inverter Mask Set

• Transistors and wires are defined by masks

• Cross-section taken along dashed line

Detailed Mask Views

• Six masks– n-well

– Polysilicon

– n+ diffusion

– p+ diffusion

– Contact

– Metal

Page 19: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

19

Fabrication• Chips are built in huge factories called fabs

• Contain clean rooms as large as football fields

Courtesy of International

Business Machines Corporation.

Unauthorized use not permitted.

Fabrication Steps

• Start with blank wafer

• Build inverter from the bottom up

• First step will be to form the n-well– Cover wafer with protective layer of SiO2 (oxide)

– Remove layer where n-well should be built

– Implant or diffuse n dopants into exposed wafer

– Strip off SiO2

Page 20: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

20

Oxidation

• Grow SiO2 on top of Si wafer– 900 – 1200 C with H2O or O2 in oxidation furnace

Photoresist

• Spin on photoresist– Photoresist is a light-sensitive organic polymer

– Softens where exposed to light

Page 21: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

21

Lithography

• Expose photoresist through n-well mask

• Strip off exposed photoresist

Etch

• Etch oxide with hydrofluoric acid (HF)– Seeps through skin and eats bone; nasty stuff!!!

• Only attacks oxide where resist has been exposed

Page 22: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

22

Strip Photoresist

• Strip off remaining photoresist– Use mixture of acids called piranah etch

• Necessary so resist doesn’t melt in next step

n-well• n-well is formed with diffusion or ion implantation

• Diffusion– Place wafer in furnace with arsenic gas

– Heat until As atoms diffuse into exposed Si

• Ion Implanatation– Blast wafer with beam of As ions

– Ions blocked by SiO2, only enter exposed Si

Page 23: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

23

Strip Oxide

• Strip off the remaining oxide using HF

• Back to bare wafer with n-well

• Subsequent steps involve similar series of steps

Polysilicon• Deposit very thin layer of gate oxide

– < 20 Å (6-7 atomic layers)

• Chemical Vapor Deposition (CVD) of silicon layer– Place wafer in furnace with Silane gas (SiH4)

– Forms many small crystals called polysilicon

– Heavily doped to be good conductor

Page 24: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

24

Polysilicon Patterning

• Use same lithography process to pattern polysilicon

Self-Aligned Process• Use oxide and masking to expose where n+

dopants should be diffused or implanted

• N-diffusion forms nMOS source, drain, and n-well contact

Page 25: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

25

N-diffusion• Pattern oxide and form n+ regions

• Self-aligned process where gate blocks diffusion

• Polysilicon is better than metal for self-aligned gates because it doesn’t melt during later processing

N-diffusion cont.

• Historically dopants were diffused

• Usually ion implantation today

• But regions are still called diffusion

Page 26: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

26

N-diffusion cont.

• Strip off oxide to complete patterning step

52

P-Diffusion

• Similar set of steps form p+ diffusion regions for pMOS source and drain and substrate contact

Page 27: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

27

53

Contacts

• Now we need to wire together the devices

• Cover chip with thick field oxide

• Etch oxide where contact cuts are needed

54

Metallization• Sputter on aluminum over whole wafer

• Pattern to remove excess metal, leaving wires

Page 28: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

28

55

Design Rules• Design rules govern the layout of individual

components: transistors, wires, contacts, vias– How small can the gates be, and how small can the

wires be made?

• Conflicting Demands: – component packing: more functionality, higher speed

– Chip yield: smaller sizes can reduce yield (fraction of good chips)

• Conservative vs aggressive design rules

56

Foundry Interface

Designer

Layout(mask set)

Design RulesProcess Parameters

Foundry

Page 29: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

29

57

Layout• Chips are specified with set of masks

• Minimum dimensions of masks determine transistor size (and hence speed, cost, and power)

• Feature size f = distance between source and drain– Set by minimum width of polysilicon

• Feature size improves 30% every 3 years or so

• Normalize for feature size when describing design rules

• Express rules in terms of = f/2– E.g. = 0.3 μm in 0.6 μm process

58

Simplified Design Rules

• Conservative rules to get you started

Page 30: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

30

59

Geometric Design Rules

• Resolution– Width and spacing of lines on one layer

• Alignment– make sure interacting layers overlap (or don’t)

– Contact surround

– Poly overlap of diffusion

– Well surround of diffusion

60

SCMOS Design Rules• Scalable CMOS design rules• Feature size = half the drawn gate length (poly width)• Mentor Graphics IC tool has built-in design rule checker (DRC)

Layer Minimum Width SeparationMetal 1 3 3Metal 2 3 4Poly 2 poly-poly: 2 poly-diff: 1

Example design rules:

Page 31: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

31

61

Tub Ties and Latchup• Substrate must be connected to power supply• p-tub for nMOS to VSS (Gnd)• n-tub for pMOS to VDD

• Connections made by special vias called tub ties• Conservative design rule: place tub ties for every

one or two transistors• Why not place one tie in each tub that has 50

transistors?

62

Latchup• Too few ties: high resistance between tub and power

supply, leads to parasitic bipolar transistors inhibiting normal chip operation

• Parasitic silicon-controlled rectifier (SCR)• When both bipolar transistors are off, SCR conducts no

current• SCR turns on: high current short-circuit between VDD

and Gnd.

Page 32: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

32

63

Stick Diagrams• Designing complete layout in terms of rectangles can be

overwhelming

• Stick diagram: abstraction between transistor schematic and layout– Cartoon of a chip layout

• Replace rectangles by lines

a a

VDD

Gnd

VDD (blue)

VSS (Gnd)

a

transistor

n-typediffusion(green)

Poly (red)

p-type diffusion(yellow)

Metal 1 (blue)

64

Stick Diagram

Gnd

VDD

a

b

a b

z

n-diffusion

p-diffusion

Metal 1

Metal 1

a b

Poly

VDD

Gnd

Page 33: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

33

65

Cell Minimization• Chip area (cell size) must be minimized carefully

Impact of die size/chip area on cost (unpackaged dies)

Wafer cost $1,460 $1,460 $1,460Die size 160.2 mm2 161.8 mm2 184.2 mm2 Die cost $84.06 $85.33 $102.55Chipsfabricatedper week 498.1 K 482.9 K 337.5 K Addedannual cost $63.5 M $961 M

NominalPentium die

1% increasein die size

15% increasein die size

66

Minimize number of diffusion strips• How do we order the gate inputs (poly)?• More diffusion strips more spacing, more area

VDD

ab

c

a

F

d e

b c

d

eVDD

Gnd

Try a, b, c, d, e:

a b c d ex xx

F

x x xx

x xx

Two n-diff gaps, zero p-diff gaps

x x

Page 34: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

34

67

VDD

ab

c

a

Gnd

d e

b c

d

e

pMOS graph

a

b c

d

e

nMOS graph

b

c

a

d e

68

• Euler path: Visit every edge exactly once• Find all Euler paths for nMOS and pMOS graphs• Find p- and n-path that have identicallabeling

• For example: d, e, a, b, c • If no such path exists, then break diffusion into strips

Page 35: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

35

69

VDD

ab

c

a

Gnd

e

b c

d

e

pMOS grapha

b c

d

e

nMOS graph

b

c

a

d e

F

Ordering: d, e, a, b, c:

a b cd e

F

xx

VDD

GndZero n-diff gaps, zero p-diff gaps

d

x x x x

xx x

x

70

Some Layout Hints• Plan the global structure

(“big picture”), then design cells– Floorplan

– Wiring strategy

– Power and ground distribution

– Systematic placement

– Keep all pMOS/nMOS together

– Place transistors in rows: share source/drain diffusion

• Wiring on orthogonal metal layers– Assign preferred

directions to M1 and M2

– Use diffusion only for devices, not for interconnect

– Use poly only for very local interconnect

Page 36: MOS Transistor Theory - All Facultypeople.ee.duke.edu/~krish/teaching/Lectures/MOS_theory... · 2010-09-13 · 1 1 MOS Transistor Theory • So far, we have viewed a MOS transistor

36

71

Inverter Layout

• Transistor dimensions specified as Width / Length– Minimum size is 4 / 2 , sometimes called 1 unit

– In f = 0.6 μm process, this is 1.2 μm wide, 0.6 μm long

72

Summary

• MOS transistors are stacks of gate, oxide, silicon

• Act as electrically controlled switches

• Build logic gates out of switches

• Draw masks to specify layout of transistors

• Now you know everything necessary to start designing schematics and layout for a simple chip!