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7/27/2019 MOS Theory http://slidepdf.com/reader/full/mos-theory 1/8 ECE 261 Krish Chakrabarty 1 MOS Transistor Theory So far, we have viewed a MOS transistor as an ideal switch (digital operation)  – Reality: less than ideal ECE 261 Krish Chakrabarty 2 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)

MOS Theory

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7/27/2019 MOS Theory

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ECE 261 Krish Chakrabarty 1

MOS Transistor Theory

• So far, we have viewed a MOS transistor as an

ideal switch (digital operation)

 – Reality: less than ideal

ECE 261 Krish Chakrabarty 2

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)

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ECE 261 Krish Chakrabarty 3

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

ECE 261 Krish Chakrabarty 4

nMOS Device Behavior

Vgs << Vt

Polysilicon gate p-substrate

Accumulation

mode

• 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

Inversion

Region

(n-type)

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ECE 261 Krish Chakrabarty 5

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

ECE 261 Krish Chakrabarty 6

Threshold Voltage: Concept

n+n+

 p-substrate

 D S 

 B

VGS

+

-

Depletion

Region

n-channel

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ECE 261 Krish Chakrabarty 7

Current-Voltage Relations

n+n+

 p-substrate

D

S

G

B

V GS

 x L

V ( x )

+ –

V DS

I D

MOS transistor and its bias conditions

ECE 261 Krish Chakrabarty 8

Current-Voltage Relations

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ECE 261 Krish Chakrabarty 9

Current-Voltage Relations

k n: transconductance of transistor 

W : 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

ECE 261 Krish Chakrabarty 10

Typical Parameter Values

k Vt

n-type 24 microA/V2 0.8V

 p-type 9 microA/V2 -0.8V

Why is k higher for n-type transistors?

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ECE 261 Krish Chakrabarty 11

Transistor in Saturation

n+n+

 S 

VGS

 D

VDS > VGS - VT

VGS - VT

+-

Channel is pinched off 

ECE 261 Krish Chakrabarty 12

The Gate Capacitance

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ECE 261 Krish Chakrabarty 13

Diffusion Capacitance

ECE 261 Krish Chakrabarty 14

Parasitic Resistances

W

 L D

Drain

Draincontact

Polysilicon gate

 D S 

 RS  R D

V GS,eff  

R S = (LS/W)R + R C

R D = (LD/W)R + R C

R C: contact resistance

R : sheet resistance per square

of drain-source diffusion

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ECE 261 Krish Chakrabarty 15

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