introduction to metal-oxide-semiconductor field effect transistors (mosfets) chapter 7, anderson and...

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Introduction to Metal-Oxide- Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

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Page 1: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Introduction toMetal-Oxide-

SemiconductorField Effect Transistors

(MOSFETs)

Chapter 7, Anderson and Anderson

Page 2: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

MOSFET• History• Structure• Future• Review• Threshold Voltage• I-V Characteristics• Modifications to I-V:

– Depletion layer correction (Sup. 3)– Mobility, Vsat– Short Channel Effects– Channel Length Modulation– Channel Quantum Effects

• MOSFET Scaling and Current Topics (Literature + Sup. 3)• Subthreshold Behavior• Damage and Temperature (Sup. 3)• Spice (Sup. 3)• HFET, MESFET, JFET, DRAM, CCD (Some in Sup. 3)

Page 3: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

MOSFET History (Very Short!)

• First Patents: – 1935

• Variable Capacitor Proposed: – 1959

• Silicon MOS: – 1960

• Clean PMOS, NMOS: – Late 1960s, big growth!

• CCDs: – 1970s, Bell Labs

• Switch to CMOS: – 1980s

Page 4: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Structure: n-channel MOSFET(NMOS)

pn+n+

metal

LW

sourceS

gate: metal or heavily doped poly-Si G

drainD

bodyB

oxide

IG=0

ID=ISIS

x

y

(bulk or substrate)

Page 5: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

MOSFET Future (One Part of)

• International Technology Roadmap for Semiconductors, 2008 update.

• Look at size, manufacturing technique.

Page 6: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson
Page 7: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson
Page 8: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

From Intel

Page 9: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Structure: n-channel MOSFET(NMOS)

pn+n+

metal

LW

sourceS

gate: metal or heavily doped poly-Si G

drainD

bodyB

oxide

IG=0

ID=ISIS

x

y

(bulk or substrate)

Page 10: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson
Page 11: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

MOSFET ScalingECE G201

Page 12: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Fin (30nm)

Gate

BOX

prevents “top” gate

Page 13: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Circuit Symbol (NMOS)enhancement-type: no channel at zero gate voltage

G

D

S

B (IB=0, should be reverse biased)

ID= IS

IS

IG= 0

G-GateD-DrainS-SourceB-Substrate or Body

Page 14: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson
Page 15: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Structure: n-channel MOSFET(NMOS)

pn+n+

metal

LW

sourceS

gate: metal or heavily doped poly-Si G

drainD

bodyB

oxide

IG=0

ID=ISIS

x

y

(bulk or substrate)

Page 16: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Energy bands

(“flat band” condition; not equilibrium) (equilibrium)

Page 17: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Flatbands! For this choice of materials, VGS<0 n+pn+ structure ID ~ 0

pn+n+

n++

LW

sourceS

gateG

drainD

bodyB

oxide

+-

VD=Vs

Page 18: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Flatbands < VGS < VT (Includes VGS=0 here). n+-depletion-n+ structure ID ~ 0

pn+n+

n++

LW

sourceS

gateG

drainD

bodyB

oxide

+-

+++

VD=Vs

Page 19: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

VGS > VT n+-n-n+ structure inversion

pn+n+

n++

LW

sourceS

gateG

drainD

bodyB

oxide

+-

+++++++++

- - - - -

VD=Vs

Page 20: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

VGS>VT

Channel Charge (Qch)

Qch

Depletion regioncharge (QB) is dueto uncovered acceptor ions

Page 21: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

pn+n+

n++

LW

Ec(y) with VDS=0

(x)

Page 22: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Increasing VGS decreases EB

EB

y0 L

EF ~ EC

Page 23: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Triode Region A voltage-controlled resistor @small VDS

G

pn+n+

metal

S DB

oxide

+-

+++

+++

- - - -

VGS1>Vt

pn+n+

metal

S DB

oxide

+-

+++

++++++

- - - - - -

VGS2>VGS1

pn+n+

metal

S DB

oxide

+-

+++

++++++

- - - - - - - - -

VGS3>VGS2+++

ID

VDS

0.1 v

increasingVGS

Increasing VGS puts more charge in the channel, allowing more drain current to flow

cut-off

Page 24: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Saturation Regionoccurs at large VDS

pn+n+

metal

sourceS

gateG

drainD

bodyB

oxide

+-

+++++++++

VDS large

As the drain voltage increases, the difference in voltage between the drain and the gate becomes smaller. At some point, the difference is too small to maintain the channel near the drain pinch-off

Page 25: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Saturation Regionoccurs at large VDS

pn+n+

metal

sourceS

gateG

drainD

bodyB

oxide

+-

+++++++++

VDS large

The saturation region is when the MOSFET experiences pinch-off.

Pinch-off occurs when VG - VD is less than VT.

Page 26: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Saturation Regionoccurs at large VDS

pn+n+

metal

sourceS

gateG

drainD

bodyB

oxide

+-

+++++++++

VD>>Vs

VGS - VDS < VT or VGD <

VDS > VGS - VT

VT

Page 27: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Saturation Regiononce pinch-off occurs, there is no further increase in

drain current

ID

VDS

0.1 v

increasingVGS

triode

saturation

VDS>VGS-VT

VDS<VGS-VT

Page 28: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Band diagram of triode and saturation

Page 29: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Simplified MOSFET I-V Equations

Cut-off: VGS< VT

ID = IS = 0

Triode: VGS>VT and VDS < VGS-VT

ID = kn’(W/L)[(VGS-VT)VDS - 1/2VDS

2]

Saturation: VGS>VT and VDS > VGS-VT

ID = 1/2kn’(W/L)(VGS-VT)2

where kn’= (electron mobility)x(gate capacitance)

= n(ox/tox) …electron velocity = nE

and VT depends on the doping concentration and gate material used (…more details later)

Page 30: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Energy bands

(“flat band” condition; not equilibrium) (equilibrium)

Page 31: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson
Page 32: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

VGS>VT

Channel Charge (Qch)

Qch

Depletion regioncharge (QB) is dueto uncovered acceptor ions

Page 33: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson
Page 34: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson
Page 35: Introduction to Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) Chapter 7, Anderson and Anderson

Threshold Voltage Definition

VGS = VT when the carrier concentration in the channel is equal to the carrier concentration in the bulk silicon.

Mathematically, this occurs when s=2f ,

where s is called the surface potential