Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5...

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MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 1 Chap 5. MOS Fundamentals u Ideal Structure u Energy Band Diagram u Bias Effects u Capacitance-Voltage Characteristics u Current-Voltage Characteristics u Nonideal MOS u Gate Oxide Integrity

Transcript of Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5...

Page 1: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

1

Chap 5. MOS Fundamentals

u Ideal Structureu Energy Band Diagramu Bias Effectsu Capacitance-Voltage Characteristicsu Current-Voltage Characteristicsu Nonideal MOS u Gate Oxide Integrity

Page 2: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

2

Ideal Structure Definition

u MOS Capacitor

Page 3: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

3

Energy Band Diagram

u Individual energy band diagram

u Ideal Structure energy Band Diagram

Page 4: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

4

Block Charge Diagram

Page 5: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

5

Bias Effect

Ideal N-MOS Capacitor

Page 6: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

6

Bias Effect

Ideal P-MOS Capacitor

Page 7: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

7

C-V Characteristics

High- and low-frequency C-V characteristics of a pMOS capacitor

Page 8: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

8

AC Charge fluctuations inside an n-MOS C

VG < 0, Accumulation VG ≥ 0, Depletion

VG > 0, Inversion

Page 9: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

9

Oxide Thickness Effects

Page 10: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

10

Sweep Frequency Effects

Page 11: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

11

Nonideal MOS

u Metal-Semiconductor Workfunction Difference u Oxide Charge

– Mobile Ions– Trapped Oxide Charge– Fixed Charge– Interfacial traps

Page 12: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

12

Workfunction Difference

u Metal-Semiconductor workfunction difference induces a built-in potential (band bending) in MOS-C even when VG = 0.

u Vbi = φMS = φM - φS

Page 13: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

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Work function as a function of doping conc. of semiconductor

Page 14: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

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Barrier Height of Various Metals on MOS-Cs

Page 15: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

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Oxide Charges

Four Major Charge/Traps in SiO2Mobile IonsTrapped Oxide ChargeFixed ChargeInterfacial traps

Arbitrary distribution of oxide charges

Page 16: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

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Mobile Ions

u Arise from “Alkali-ion” contamination, such as Na+ and K+.u C-V curve shifts with bias-temperature.

∫−=

ox

ooG dxxx

kV

0)(ion

1ions

mobileρ

ε

Page 17: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

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Mobile Ions

u Two hypothetical ionic charge distributions involving the same total number of ions situated near the metal and near the semiconductor.

u Positive mobile ions within the oxide under (+) and (-) bias-temperature stressing.

u Specail fabrication procedures needed, such as RCA clean, Phosphorus or chlorine stabilization, and extremely clean environment.

Page 18: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

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MOS stabilization procedures

Page 19: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

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Fixed Charge

o

FG C

QV −=

charge

fixedDue to excess ionic silicon that has broken away the silicon proper and is waiting to react in the vicinity of the Si-SiO2 interface when the oxidation process is abruptly terminated.

Page 20: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

20

Effects of oxidation process on fixed charge

Page 21: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

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Interfacial Traps

u Interfacial traps are allowed energy states in which electrons are localized in the vicinity of Si-SiO2 interface. ⇒C-V curve distortion

Page 22: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

22

Interfacial Traps

Page 23: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

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Physical Model of Interfacial traps

Page 24: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

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Energy Distribution of Interface states

Annihilation of interface states by postmetallization H2annealing

Page 25: Chap 5. MOS Fundamentalsweng/courses/IC_2007/PROJECT_… · MOS Device Physics and Designs Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 19 Fixed Charge o F G C Q V −= ∆ charge

MOS Device Physics and Designs Chap. 5

Instructor: Pei-Wen LiDept. of E. E. NCU

25

Induced Charge

u Radiation effects: a major concern of space and military.

∆VG Summary ( ) ( )o

SIT

o

MM

o

FMSGGG C

QC

QCQVVV φγ

φφ

−−−=−=∆S same

'