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Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS MOSFET Transistor Structure and I/V Characteristics Dr. Alaa El-Din Hussein March 21, 2008 Dr. Alaa El-Din Hussein — MOSFET Transistor 1/29

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Page 1: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

MOSFET TransistorStructure and I/V Characteristics

Dr. Alaa El-Din Hussein

March 21, 2008

Dr. Alaa El-Din Hussein — MOSFET Transistor 1/29

Page 2: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Outline

1 Enhancement NMOS Structure

2 Qualitative I/V C/Cs

3 I/V C/Cs

4 Depletion NMOS Transistor

5 Enhancement PMOS Transistor

6 CMOS

Dr. Alaa El-Din Hussein — MOSFET Transistor 2/29

Page 3: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Outline

1 Enhancement NMOS Structure

2 Qualitative I/V C/Cs

3 I/V C/Cs

4 Depletion NMOS Transistor

5 Enhancement PMOS Transistor

6 CMOS

Dr. Alaa El-Din Hussein — MOSFET Transistor 3/29

Page 4: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Enhancement NMOS Structure

Notes

4 device terminals: Gate(G), Drain(D), Source(S) and Body(B).

Source and drain regions form PN junctions with substrate.

VSB , VDS , and VGS always positive during normal operation.

VSB always < VDS and VGS to reverse bias PN junctions

Dr. Alaa El-Din Hussein — MOSFET Transistor 4/29

Page 5: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Enhancement NMOS Structure

Notes

4 device terminals: Gate(G), Drain(D), Source(S) and Body(B).

Source and drain regions form PN junctions with substrate.

VSB , VDS , and VGS always positive during normal operation.

VSB always < VDS and VGS to reverse bias PN junctions

Dr. Alaa El-Din Hussein — MOSFET Transistor 4/29

Page 6: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Enhancement NMOS Structure

Notes

4 device terminals: Gate(G), Drain(D), Source(S) and Body(B).

Source and drain regions form PN junctions with substrate.

VSB , VDS , and VGS always positive during normal operation.

VSB always < VDS and VGS to reverse bias PN junctions

Dr. Alaa El-Din Hussein — MOSFET Transistor 4/29

Page 7: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Enhancement NMOS Structure

Notes

4 device terminals: Gate(G), Drain(D), Source(S) and Body(B).

Source and drain regions form PN junctions with substrate.

VSB , VDS , and VGS always positive during normal operation.

VSB always < VDS and VGS to reverse bias PN junctions

Dr. Alaa El-Din Hussein — MOSFET Transistor 4/29

Page 8: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Enhancement NMOS Structure

Notes

4 device terminals: Gate(G), Drain(D), Source(S) and Body(B).

Source and drain regions form PN junctions with substrate.

VSB , VDS , and VGS always positive during normal operation.

VSB always < VDS and VGS to reverse bias PN junctions

Dr. Alaa El-Din Hussein — MOSFET Transistor 4/29

Page 9: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Outline

1 Enhancement NMOS Structure

2 Qualitative I/V C/Cs

3 I/V C/Cs

4 Depletion NMOS Transistor

5 Enhancement PMOS Transistor

6 CMOS

Dr. Alaa El-Din Hussein — MOSFET Transistor 5/29

Page 10: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Qualitative I/V CharacteristicsGate Voltage equals zero

Notes

VGS << VTN (Threshold Voltage): Two back-to-back diodes existsin series between source and drain. Only small leakage current flows.

Please note: In the text-book Vt is used for the threshold voltage toavoid confusion with the thermal voltage (VT ). We will use eitherVt or( VTN (n-device) and VTP (P device))

iB=0 and iG =0.

Dr. Alaa El-Din Hussein — MOSFET Transistor 6/29

Page 11: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Qualitative I/V CharacteristicsGate Voltage equals zero

Notes

VGS << VTN (Threshold Voltage): Two back-to-back diodes existsin series between source and drain. Only small leakage current flows.

Please note: In the text-book Vt is used for the threshold voltage toavoid confusion with the thermal voltage (VT ). We will use eitherVt or( VTN (n-device) and VTP (P device))

iB=0 and iG =0.

Dr. Alaa El-Din Hussein — MOSFET Transistor 6/29

Page 12: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Qualitative I/V CharacteristicsGate Voltage equals zero

Notes

VGS << VTN (Threshold Voltage): Two back-to-back diodes existsin series between source and drain. Only small leakage current flows.

Please note: In the text-book Vt is used for the threshold voltage toavoid confusion with the thermal voltage (VT ). We will use eitherVt or( VTN (n-device) and VTP (P device))

iB=0 and iG =0.

Dr. Alaa El-Din Hussein — MOSFET Transistor 6/29

Page 13: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Qualitative I/V CharacteristicsGate Voltage equals zero

Notes

VGS << VTN (Threshold Voltage): Two back-to-back diodes existsin series between source and drain. Only small leakage current flows.

Please note: In the text-book Vt is used for the threshold voltage toavoid confusion with the thermal voltage (VT ). We will use eitherVt or( VTN (n-device) and VTP (P device))

iB=0 and iG =0.

Dr. Alaa El-Din Hussein — MOSFET Transistor 6/29

Page 14: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Qualitative I/V CharacteristicsSub-Threshold Operation VGS < VTN

Notes

VGS < VTN : Depletion region formed under gate merges with sourceand drain depletion regions.

No current flows between source and drain.

iB=0 and iG =0.

Dr. Alaa El-Din Hussein — MOSFET Transistor 7/29

Page 15: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Qualitative I/V CharacteristicsSub-Threshold Operation VGS < VTN

Notes

VGS < VTN : Depletion region formed under gate merges with sourceand drain depletion regions.

No current flows between source and drain.

iB=0 and iG =0.

Dr. Alaa El-Din Hussein — MOSFET Transistor 7/29

Page 16: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Qualitative I/V CharacteristicsSub-Threshold Operation VGS < VTN

Notes

VGS < VTN : Depletion region formed under gate merges with sourceand drain depletion regions.

No current flows between source and drain.

iB=0 and iG =0.

Dr. Alaa El-Din Hussein — MOSFET Transistor 7/29

Page 17: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Qualitative I/V CharacteristicsSub-Threshold Operation VGS < VTN

Notes

VGS < VTN : Depletion region formed under gate merges with sourceand drain depletion regions.

No current flows between source and drain.

iB=0 and iG =0.

Dr. Alaa El-Din Hussein — MOSFET Transistor 7/29

Page 18: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Qualitative I/V CharacteristicsThreshold Operation VGS > VTN

Notes

VGS > VTN : Channel formed between source and drain.

If vDS > 0, finite iD flows from drain to source.

iB=0 and iG =0.

Dr. Alaa El-Din Hussein — MOSFET Transistor 8/29

Page 19: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Qualitative I/V CharacteristicsThreshold Operation VGS > VTN

Notes

VGS > VTN : Channel formed between source and drain.

If vDS > 0, finite iD flows from drain to source.

iB=0 and iG =0.

Dr. Alaa El-Din Hussein — MOSFET Transistor 8/29

Page 20: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Qualitative I/V CharacteristicsThreshold Operation VGS > VTN

Notes

VGS > VTN : Channel formed between source and drain.

If vDS > 0, finite iD flows from drain to source.

iB=0 and iG =0.

Dr. Alaa El-Din Hussein — MOSFET Transistor 8/29

Page 21: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Qualitative I/V CharacteristicsThreshold Operation VGS > VTN

Notes

VGS > VTN : Channel formed between source and drain.

If vDS > 0, finite iD flows from drain to source.

iB=0 and iG =0.

Dr. Alaa El-Din Hussein — MOSFET Transistor 8/29

Page 22: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

Outline

1 Enhancement NMOS Structure

2 Qualitative I/V C/Cs

3 I/V C/Cs

4 Depletion NMOS Transistor

5 Enhancement PMOS Transistor

6 CMOS

Dr. Alaa El-Din Hussein — MOSFET Transistor 9/29

Page 23: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsLinear (Triode) Region

iD = Kn

(vGS − VTN −

vDS

2

)vDS

where, Kn = K′nW/L, K′

n = µnCox (A/V 2), Cox = εox/Tox , εox =oxide permittivity (F/cm), Tox =oxide thickness (cm)

Channel current is drift

Output characteristics appear to be linear.

FET behaves like a gate-source voltage-controlled resistor betweensource and drain with Ron = 1

K ′n

WL (VGS−VTN )

Dr. Alaa El-Din Hussein — MOSFET Transistor 10/29

Page 24: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsLinear (Triode) Region

iD = Kn

(vGS − VTN −

vDS

2

)vDS

where, Kn = K′nW/L, K′

n = µnCox (A/V 2), Cox = εox/Tox , εox =oxide permittivity (F/cm), Tox =oxide thickness (cm)

Channel current is drift

Output characteristics appear to be linear.

FET behaves like a gate-source voltage-controlled resistor betweensource and drain with Ron = 1

K ′n

WL (VGS−VTN )

Dr. Alaa El-Din Hussein — MOSFET Transistor 10/29

Page 25: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsLinear (Triode) Region

iD = Kn

(vGS − VTN −

vDS

2

)vDS

where, Kn = K′nW/L, K′

n = µnCox (A/V 2), Cox = εox/Tox , εox =oxide permittivity (F/cm), Tox =oxide thickness (cm)

Channel current is drift

Output characteristics appear to be linear.

FET behaves like a gate-source voltage-controlled resistor betweensource and drain with Ron = 1

K ′n

WL (VGS−VTN )

Dr. Alaa El-Din Hussein — MOSFET Transistor 10/29

Page 26: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsLinear (Triode) Region

iD = Kn

(vGS − VTN −

vDS

2

)vDS

where, Kn = K′nW/L, K′

n = µnCox (A/V 2), Cox = εox/Tox , εox =oxide permittivity (F/cm), Tox =oxide thickness (cm)

Channel current is drift

Output characteristics appear to be linear.

FET behaves like a gate-source voltage-controlled resistor betweensource and drain with Ron = 1

K ′n

WL (VGS−VTN )

Dr. Alaa El-Din Hussein — MOSFET Transistor 10/29

Page 27: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsLinear (Triode) Region

iD = Kn

(vGS − VTN −

vDS

2

)vDS

where, Kn = K′nW/L, K′

n = µnCox (A/V 2), Cox = εox/Tox , εox =oxide permittivity (F/cm), Tox =oxide thickness (cm)

Channel current is drift

Output characteristics appear to be linear.

FET behaves like a gate-source voltage-controlled resistor betweensource and drain with Ron = 1

K ′n

WL (VGS−VTN )

Dr. Alaa El-Din Hussein — MOSFET Transistor 10/29

Page 28: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsExample: Voltage-Controlled Attenuator

Example

Calculate vo , givenKn = 500µA/V 2,VTN = 1V ,R = 2kΩ,VGG = 1.5V and vs = 0.5V

Using VDR we can write: vo

vs= Ron

Ron+R = 11+KnR(VGG−VTN )

Substitute by the given values: vo = 0.51+500µA

V 2 (2000Ω)(1.5−1)V= 0.33V

Dr. Alaa El-Din Hussein — MOSFET Transistor 11/29

Page 29: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsExample: Voltage-Controlled Attenuator

Example

Calculate vo , givenKn = 500µA/V 2,VTN = 1V ,R = 2kΩ,VGG = 1.5V and vs = 0.5V

Using VDR we can write: vo

vs= Ron

Ron+R = 11+KnR(VGG−VTN )

Substitute by the given values: vo = 0.51+500µA

V 2 (2000Ω)(1.5−1)V= 0.33V

Dr. Alaa El-Din Hussein — MOSFET Transistor 11/29

Page 30: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsExample: Voltage-Controlled Attenuator

Example

Calculate vo , givenKn = 500µA/V 2,VTN = 1V ,R = 2kΩ,VGG = 1.5V and vs = 0.5V

Using VDR we can write: vo

vs= Ron

Ron+R = 11+KnR(VGG−VTN )

Substitute by the given values: vo = 0.51+500µA

V 2 (2000Ω)(1.5−1)V= 0.33V

Dr. Alaa El-Din Hussein — MOSFET Transistor 11/29

Page 31: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsExample: Voltage-Controlled Attenuator

Example

Calculate vo , givenKn = 500µA/V 2,VTN = 1V ,R = 2kΩ,VGG = 1.5V and vs = 0.5V

Using VDR we can write: vo

vs= Ron

Ron+R = 11+KnR(VGG−VTN )

Substitute by the given values: vo = 0.51+500µA

V 2 (2000Ω)(1.5−1)V= 0.33V

Dr. Alaa El-Din Hussein — MOSFET Transistor 11/29

Page 32: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsLinear (Triode) Region

If vDS is small the channel (inversion layer) will be uniform and thetransistor will be in the linear or triode region as studied before.

Dr. Alaa El-Din Hussein — MOSFET Transistor 12/29

Page 33: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsLinear (Triode) Region

If vDS is small the channel (inversion layer) will be uniform and thetransistor will be in the linear or triode region as studied before.

Dr. Alaa El-Din Hussein — MOSFET Transistor 12/29

Page 34: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsVDS = VDsat = VGS − VTN

If VDS is increased the channel (inversion layer) will be tapered nearthe drain and it will disappear when VDS = VDsat = VGS − VTN .

Dr. Alaa El-Din Hussein — MOSFET Transistor 13/29

Page 35: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsVDS = VDsat = VGS − VTN

If VDS is increased the channel (inversion layer) will be tapered nearthe drain and it will disappear when VDS = VDsat = VGS − VTN .

Dr. Alaa El-Din Hussein — MOSFET Transistor 13/29

Page 36: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsSaturation Region

If vDS increases above triode region limit, channel region disappears,also said to be pinched-off.

Current saturates at constant value, independent of vDS .

Saturation region operation mostly used for analog amplification.

The current will be given by:iD =K ′

n

2WL (vGS − VTN)2

Dr. Alaa El-Din Hussein — MOSFET Transistor 14/29

Page 37: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsSaturation Region

If vDS increases above triode region limit, channel region disappears,also said to be pinched-off.

Current saturates at constant value, independent of vDS .

Saturation region operation mostly used for analog amplification.

The current will be given by:iD =K ′

n

2WL (vGS − VTN)2

Dr. Alaa El-Din Hussein — MOSFET Transistor 14/29

Page 38: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsSaturation Region

If vDS increases above triode region limit, channel region disappears,also said to be pinched-off.

Current saturates at constant value, independent of vDS .

Saturation region operation mostly used for analog amplification.

The current will be given by:iD =K ′

n

2WL (vGS − VTN)2

Dr. Alaa El-Din Hussein — MOSFET Transistor 14/29

Page 39: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsSaturation Region

If vDS increases above triode region limit, channel region disappears,also said to be pinched-off.

Current saturates at constant value, independent of vDS .

Saturation region operation mostly used for analog amplification.

The current will be given by:iD =K ′

n

2WL (vGS − VTN)2

Dr. Alaa El-Din Hussein — MOSFET Transistor 14/29

Page 40: MOSFET Transistor - Structure and I/V Characteristics · 2018-03-14 · Enhancement NMOS StructureQualitative I/V C/CsI/V C/CsDepletion NMOS TransistorEnhancement PMOS TransistorCMOS

Enhancement NMOS Structure Qualitative I/V C/Cs I/V C/Cs Depletion NMOS Transistor Enhancement PMOS Transistor CMOS

NMOS Enhancement I/V CharacteristicsSaturation Region

If vDS increases above triode region limit, channel region disappears,also said to be pinched-off.

Current saturates at constant value, independent of vDS .

Saturation region operation mostly used for analog amplification.

The current will be given by:iD =K ′

n

2WL (vGS − VTN)2

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NMOS Enhancement I/V CharacteristicsID − VDS Characteristics

The current is given by: iD = K ′nWL

(vGS − Vt − vDS

2

)vDS for

vGS − Vt ≥ vDS ≥ 0

The current is given by:iD =K ′

n

2WL (vGS − Vt)2 for vGS − Vt ≤ vDS

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NMOS Enhancement I/V CharacteristicsID − VDS Characteristics

The current is given by: iD = K ′nWL

(vGS − Vt − vDS

2

)vDS for

vGS − Vt ≥ vDS ≥ 0

The current is given by:iD =K ′

n

2WL (vGS − Vt)2 for vGS − Vt ≤ vDS

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NMOS Enhancement I/V CharacteristicsID − VDS Characteristics

The current is given by: iD = K ′nWL

(vGS − Vt − vDS

2

)vDS for

vGS − Vt ≥ vDS ≥ 0

The current is given by:iD =K ′

n

2WL (vGS − Vt)2 for vGS − Vt ≤ vDS

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NMOS Enhancement I/V CharacteristicsChannel Length Modulation

Notes

As vDS increases above vDSAT , the length of the depleted channelbeyond pinch-off point, ∆L, increases and actual L decreases.

iD increases slightly with vDS instead of being constant.

To include this effect the current at saturation may be rewritten as:

iD =K ′

n

2WL (vGS − VTN)2 (1 + λvDS), where λ is called channel

length modulation parameter.

In other words the output resistance at saturation will be finiteequals 1

λ.ID.

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NMOS Enhancement I/V CharacteristicsChannel Length Modulation

Notes

As vDS increases above vDSAT , the length of the depleted channelbeyond pinch-off point, ∆L, increases and actual L decreases.

iD increases slightly with vDS instead of being constant.

To include this effect the current at saturation may be rewritten as:

iD =K ′

n

2WL (vGS − VTN)2 (1 + λvDS), where λ is called channel

length modulation parameter.

In other words the output resistance at saturation will be finiteequals 1

λ.ID.

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NMOS Enhancement I/V CharacteristicsChannel Length Modulation

Notes

As vDS increases above vDSAT , the length of the depleted channelbeyond pinch-off point, ∆L, increases and actual L decreases.

iD increases slightly with vDS instead of being constant.

To include this effect the current at saturation may be rewritten as:

iD =K ′

n

2WL (vGS − VTN)2 (1 + λvDS), where λ is called channel

length modulation parameter.

In other words the output resistance at saturation will be finiteequals 1

λ.ID.

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NMOS Enhancement I/V CharacteristicsChannel Length Modulation

Notes

As vDS increases above vDSAT , the length of the depleted channelbeyond pinch-off point, ∆L, increases and actual L decreases.

iD increases slightly with vDS instead of being constant.

To include this effect the current at saturation may be rewritten as:

iD =K ′

n

2WL (vGS − VTN)2 (1 + λvDS), where λ is called channel

length modulation parameter.

In other words the output resistance at saturation will be finiteequals 1

λ.ID.

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NMOS Enhancement I/V CharacteristicsChannel Length Modulation

Notes

As vDS increases above vDSAT , the length of the depleted channelbeyond pinch-off point, ∆L, increases and actual L decreases.

iD increases slightly with vDS instead of being constant.

To include this effect the current at saturation may be rewritten as:

iD =K ′

n

2WL (vGS − VTN)2 (1 + λvDS), where λ is called channel

length modulation parameter.

In other words the output resistance at saturation will be finiteequals 1

λ.ID.

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NMOS Enhancement I/V CharacteristicsEffect of Channel Length Modulation on ID − VDS

Notes

iD increases slightly with vDS instead of being constant.

iD =K ′

n

2WL (vGS − VTN)2 (1 + λvDS).

Output resistance = 1λ.ID

.

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NMOS Enhancement I/V CharacteristicsEffect of Channel Length Modulation on ID − VDS

Notes

iD increases slightly with vDS instead of being constant.

iD =K ′

n

2WL (vGS − VTN)2 (1 + λvDS).

Output resistance = 1λ.ID

.

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NMOS Enhancement I/V CharacteristicsSaturation Large Signal Model

Figure: No Channel Length Modulation

Figure: No Channel Length Modulation

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NMOS Enhancement I/V CharacteristicsBody Effect or Substrate Sensitivity

Notes

Non-zero vSB changes threshold voltage.

This substrate sensitivity may be modeled by modeled by:VTN = VTO + γ

(√vSB + 2ϕF −

√2ϕF

)Where: VTO is the zero

substrate bias for VTN (V), γ is the body-effect parameter (√

V ),and 2ϕF is the surface potential parameter (V)

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NMOS Enhancement I/V CharacteristicsBody Effect or Substrate Sensitivity

Notes

Non-zero vSB changes threshold voltage.

This substrate sensitivity may be modeled by modeled by:VTN = VTO + γ

(√vSB + 2ϕF −

√2ϕF

)Where: VTO is the zero

substrate bias for VTN (V), γ is the body-effect parameter (√

V ),and 2ϕF is the surface potential parameter (V)

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NMOS Enhancement I/V CharacteristicsBody Effect or Substrate Sensitivity

Notes

Non-zero vSB changes threshold voltage.

This substrate sensitivity may be modeled by modeled by:VTN = VTO + γ

(√vSB + 2ϕF −

√2ϕF

)Where: VTO is the zero

substrate bias for VTN (V), γ is the body-effect parameter (√

V ),and 2ϕF is the surface potential parameter (V)

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Outline

1 Enhancement NMOS Structure

2 Qualitative I/V C/Cs

3 I/V C/Cs

4 Depletion NMOS Transistor

5 Enhancement PMOS Transistor

6 CMOS

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NMOS Depletion Mode TransistorDevice Structure

Notes

NMOS transistors with with VTN ≤ 0

Ion implantation process used to form a built-in n-type channel indevice to connect source and drain by a resistive channel

Non-zero drain current for vGS = 0, negative vGS = 0 required toturn device off.

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NMOS Depletion Mode TransistorDevice Structure

Notes

NMOS transistors with with VTN ≤ 0

Ion implantation process used to form a built-in n-type channel indevice to connect source and drain by a resistive channel

Non-zero drain current for vGS = 0, negative vGS = 0 required toturn device off.

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NMOS Depletion Mode TransistorDevice Structure

Notes

NMOS transistors with with VTN ≤ 0

Ion implantation process used to form a built-in n-type channel indevice to connect source and drain by a resistive channel

Non-zero drain current for vGS = 0, negative vGS = 0 required toturn device off.

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NMOS Depletion Mode TransistorDevice Structure

Notes

NMOS transistors with with VTN ≤ 0

Ion implantation process used to form a built-in n-type channel indevice to connect source and drain by a resistive channel

Non-zero drain current for vGS = 0, negative vGS = 0 required toturn device off.

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NMOS Depletion Mode TransistorID − VGS (Input) Characteristics

Notes

VTN ≤ 0

Non-zero drain current for vGS = 0, negative vGS = 0 required toturn device off.

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NMOS Depletion Mode TransistorID − VGS (Input) Characteristics

Notes

VTN ≤ 0

Non-zero drain current for vGS = 0, negative vGS = 0 required toturn device off.

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NMOS Depletion Mode TransistorID − VDS (Output)Characteristics

Notes

VTN = −4 in this example

Non-zero drain current for vGS = 0, negative vGS = 0 required toturn device off.

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NMOS Depletion Mode TransistorID − VDS (Output)Characteristics

Notes

VTN = −4 in this example

Non-zero drain current for vGS = 0, negative vGS = 0 required toturn device off.

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NMOS Depletion Mode TransistorID − VGS Characteristics Comparison

Notes

Vt is positive for Enhancement NMOS and Depletion PMOS

Vt is negative for Depletion NMOS and Enhancement PMOS

Non-zero drain current for vGS = 0 for Depletion transistors(Normally ON).

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NMOS Depletion Mode TransistorID − VGS Characteristics Comparison

Notes

Vt is positive for Enhancement NMOS and Depletion PMOS

Vt is negative for Depletion NMOS and Enhancement PMOS

Non-zero drain current for vGS = 0 for Depletion transistors(Normally ON).

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Outline

1 Enhancement NMOS Structure

2 Qualitative I/V C/Cs

3 I/V C/Cs

4 Depletion NMOS Transistor

5 Enhancement PMOS Transistor

6 CMOS

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Enhancement PMOS TransistorDevice Structure

Notes

P-type source and drain regions in n-type substrate.

vGS < 0 required to create p-type inversion layer in channel region

For current flow, vGS < vTP

To maintain reverse bias on source-substrate and drain-substratejunctions, vSB < 0 and vDB < 0

Positive bulk-source potential causes VTP to become more negative

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Enhancement PMOS TransistorDevice Structure

Notes

P-type source and drain regions in n-type substrate.

vGS < 0 required to create p-type inversion layer in channel region

For current flow, vGS < vTP

To maintain reverse bias on source-substrate and drain-substratejunctions, vSB < 0 and vDB < 0

Positive bulk-source potential causes VTP to become more negative

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Enhancement PMOS TransistorDevice Structure

Notes

P-type source and drain regions in n-type substrate.

vGS < 0 required to create p-type inversion layer in channel region

For current flow, vGS < vTP

To maintain reverse bias on source-substrate and drain-substratejunctions, vSB < 0 and vDB < 0

Positive bulk-source potential causes VTP to become more negative

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Enhancement PMOS TransistorDevice Structure

Notes

P-type source and drain regions in n-type substrate.

vGS < 0 required to create p-type inversion layer in channel region

For current flow, vGS < vTP

To maintain reverse bias on source-substrate and drain-substratejunctions, vSB < 0 and vDB < 0

Positive bulk-source potential causes VTP to become more negative

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Enhancement PMOS TransistorDevice Structure

Notes

P-type source and drain regions in n-type substrate.

vGS < 0 required to create p-type inversion layer in channel region

For current flow, vGS < vTP

To maintain reverse bias on source-substrate and drain-substratejunctions, vSB < 0 and vDB < 0

Positive bulk-source potential causes VTP to become more negative

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Enhancement PMOS TransistorDevice Structure

Notes

P-type source and drain regions in n-type substrate.

vGS < 0 required to create p-type inversion layer in channel region

For current flow, vGS < vTP

To maintain reverse bias on source-substrate and drain-substratejunctions, vSB < 0 and vDB < 0

Positive bulk-source potential causes VTP to become more negative

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Enhancement PMOS TransistorID − VDS (Output) Characteristics

Notes

For VGS ≥ VTP or (VSG ≤ |VTP |) the transistor is off.

For more negative vGS , drain current increases in magnitude.

PMOS equations are the same as NMOS. However, we have toinvert suffixes and use |VTP | instead of |VTN | as |VTP | is –ve. Also,K ′n is replaced by K ′p = µpCox

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Enhancement PMOS TransistorID − VDS (Output) Characteristics

Notes

For VGS ≥ VTP or (VSG ≤ |VTP |) the transistor is off.

For more negative vGS , drain current increases in magnitude.

PMOS equations are the same as NMOS. However, we have toinvert suffixes and use |VTP | instead of |VTN | as |VTP | is –ve. Also,K ′n is replaced by K ′p = µpCox

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Enhancement PMOS TransistorID − VDS (Output) Characteristics

Notes

For VGS ≥ VTP or (VSG ≤ |VTP |) the transistor is off.

For more negative vGS , drain current increases in magnitude.

PMOS equations are the same as NMOS. However, we have toinvert suffixes and use |VTP | instead of |VTN | as |VTP | is –ve. Also,K ′n is replaced by K ′p = µpCox

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Enhancement PMOS TransistorID − VDS (Output) Characteristics

Notes

For VGS ≥ VTP or (VSG ≤ |VTP |) the transistor is off.

For more negative vGS , drain current increases in magnitude.

PMOS equations are the same as NMOS. However, we have toinvert suffixes and use |VTP | instead of |VTN | as |VTP | is –ve. Also,K ′n is replaced by K ′p = µpCox

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Outline

1 Enhancement NMOS Structure

2 Qualitative I/V C/Cs

3 I/V C/Cs

4 Depletion NMOS Transistor

5 Enhancement PMOS Transistor

6 CMOS

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Complementary MOS (CMOS)Structure

Notes

The CMOS is consisted of NMOS and PMOS transistors.

It is widely used in digital systems thanks to its low power dissipation

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Complementary MOS (CMOS)Structure

Notes

The CMOS is consisted of NMOS and PMOS transistors.

It is widely used in digital systems thanks to its low power dissipation

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Complementary MOS (CMOS)Structure

Notes

The CMOS is consisted of NMOS and PMOS transistors.

It is widely used in digital systems thanks to its low power dissipation

Dr. Alaa El-Din Hussein — MOSFET Transistor 29/29