Lecture #39

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OUTLINE The MOSFET: Sub-threshold leakage current Gate-length scaling. Lecture #39. We had previously assumed that there is no channel current when V GS < V T . This is incorrect. - PowerPoint PPT Presentation

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EE130 Lecture 39, Slide 1Spring 2007

Lecture #39

OUTLINE

The MOSFET:• Sub-threshold leakage current• Gate-length scaling

EE130 Lecture 39, Slide 2Spring 2007

Sub-Threshold Leakage Current• We had previously assumed that there is no channel current when VGS < VT. This is incorrect.

• If S > F, there is some inversion charge at the surface, which gives rise to sub-threshold current flowing between the source and drain:

)1()1( //)(2

kTqVmkTVVqoxeeffDS

DSTG eeqkTm

LWCI

EE130 Lecture 39, Slide 3Spring 2007

Sub-Threshold Slope S

)1)(10(ln

)(log1

10

oxe

dm

GS

DS

CC

qkT

dVIdS

EE130 Lecture 39, Slide 4Spring 2007

How to minimize S?

EE130 Lecture 39, Slide 5Spring 2007

MOSFET Scaling• MOSFETs have scaled in size over time

– 1970’s: ~ 10 m– Today: ~50 nm

• Reasons:– Speed– Density

EE130 Lecture 39, Slide 6Spring 2007

– IDS as L (decreased effective “R”)– Gate area as L (decreased load “C”)– Therefore, RC (implies faster switch)

Benefit of Transistor Scaling

EE130 Lecture 39, Slide 7Spring 2007

C C

V1 V2 V3

Vdd

Vdd

0

V2

V1

t

V32d

...........

............ (a)

(b) delaynpropagatio:d

Circuit Example – CMOS Inverter

EE130 Lecture 39, Slide 8Spring 2007

dsatN

dd

dsatP

dd

d

ICVdelaydownpull

ICVdelayuppull

delayuppulldelaydownpull

2

2

)(21

)11(4 dsatPdsatN

ddd IICV

)|(|22and

ddgdsat

dd

on

ddPN VVI

VIVRR

d is reduced by increasing IDsat

EE130 Lecture 39, Slide 9Spring 2007

Constant-Field Scaling• Voltages and MOSFET dimensions are scaled by the

same factor >1, so that the electric field remains unchanged

EE130 Lecture 39, Slide 10Spring 2007

Constant-Field Scaling (cont.)

• Circuit speed improves by

• Power dissipation per function is reduced by 2

EE130 Lecture 39, Slide 11Spring 2007

VT Design Trade-Off

• Low VT is desirable for high ON current:IDsat (VDD - VT) 1 < < 2

• But high VT is needed for low OFF current:

VT cannot be scaled aggressively!

Low VT

High VT

IOFF,high VT

IOFF,low VT

VGS

log IDS

0

EE130 Lecture 39, Slide 12Spring 2007

• Since VT cannot be scaled down aggressively, the power-supply voltage (VDD) has not been scaled down in proportion to the MOSFET channel length

EE130 Lecture 39, Slide 13Spring 2007

Generalized Scaling• Electric field intensity increases by a factor >1• Nbody must be scaled up by to control short-channel effects

• Reliability and power density are issues

EE130 Lecture 39, Slide 14Spring 2007

CMOS Scaling and the Power Crisis

1E-05

1E-04

1E-03

1E-02

1E-01

1E+00

1E+01

1E+02

1E+03

0.01 0.1 1

Gate Length (μm)Po

wer

(W/c

m2 )

Passive Power Density

Active Power Density

Lg/VDD/VT trends increases in:• Active Power Density (VDD

2) ~1.3X/generation

• Passive Power Density (VDD) ~3X/generation• Gate Leakage Power Density >4X/generation

Source: B. Meyerson, IBM, Semico Conf., January 2004