場效電晶體原理

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1. 2. MOSFET( 3. MOSFET 4. 5. MOSFET 6. MOSFET2nd order effect 7. JFET

5-1

(transistor) (valve) (a) (b)

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1

bipolar junction transistor, BJT field effect transistor, FET BJT pn B C

E p+

p C

E

n B

E B

C

VEB

VBC 5-3

FET

(channel)

S G D

S

G D

pFET

nFET

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2

FET(Junction Field Effect Transistor, JFET)(Metal-Oxide-Semiconductor FET, MOSFET)(Gate)2 (Source) n p+ L p+ (Gate)1 t (Drain) (S) (Oxide) (G)

(Metal) p n+ n+ (D) (Semiconductor) (Body)

JFET\pn

MOSFETMOS 5-5

HONOR LIST BJTpoint contact transistor Bell Laboratory(John Bardeen, 1908-1991)Walter Brattain, 1902-1987William Shockley, 1910-19891947 pn1956FETBJT FET FET

1985K. von KlitzingMOSFET (Integer Quantum Hall Effect, IQHE) 1998(HEMT, high mobility transistor) Fractional Quantum Hall Effect) , "", , , 2000. 2000 (Zhores I. Alferov)(Herbert Kroemer) (Jack St. Clair Kilby) 5-6

3

1964 for fundamental work in the field of quantum electronics, which has led to the construction of oscillators and amplifiers based on the maser-laser principle Charles Hard Townes, Nicolay Gennadiyevich Basov, Aleksandr Mikhailovich Prokhorov 1973L. Esaki (tunneling effect)

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MOSFETnMOSFET(NMOS) (S) (Oxide) (G) (S) (D) (G) (G)

(Metal) p n+ n+ (D) (Semiconductor) (Body)

(S) (body)

(D)

MOSFET MOSFET

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4

pnNMOS(cut off) (S) n+ (G) C p (Body) VDS>0

VGS=0 (Oxide) (D) n + n+

C p

S

D G IG=0

ID

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VGS

p NMOS (S) n+ p (G) n+

0Vt DS VDS DSI-V 1.0 ID 0.8 (mA) 0.6 0.4 0.2 0 0 0.2 0.4 VDS (V) VGS= 4V 3.5V 3.0V 2.5V VGS2.0V= Vt

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(a) VG VS n+ L n+ n+ C VGS Vt VG VGD VD VS VGS

(b)Vt VGD VDS VD

C n+

ID

ID

VDS

VDS 5-14

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(c) VG VS n+ VGS Vt VGD VDS n+ n+ C VG VD VS VGS

(d)VGD Vt VDS X C VD

L n+

triode ID ID

saturationVDSS

VDS

VDS

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VGD= Vt(pinch off)VDS VGDVtDL L0 0.8 (mA) 0.6 -1.0V 0.4 -1.5V VGS-2.0V 0.2 S D ID 0 G VGS