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TEORI DASAR HUBUNGAN SEMIKONDUKTOR

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Presentation on theme: "TEORI DASAR HUBUNGAN SEMIKONDUKTOR"— Presentation transcript:

1 TEORI DASAR HUBUNGAN SEMIKONDUKTOR
Hamzah Afandi, Antonius Irianto dan Betty Savitri Source: Millman, Jacob, Grabel, Arvin, Microelectronics, Mc. Graw Hill Int. Ed., 1994. Robert Boylestad, Louis Nashelsky Sixth Edition; Prentice Hall,1997.

2 Review: Semiconductor Properties Variation
Intrisic Concentration vs Temperature: Mobility vs Temperature: ; mn=2.5, mp=2.7 (100<T<400K) Mobility vs Electric Field intensity: ~ 107 cm/s 103 V/cm 104 V/cm

3 Review: Currents in semiconductor
Drift Current: Drill: Calculate the conductivity of an extrinsic semiconductor with donor atom’s concentration of 1016 atom/cm3 (at 300K)!

4 Charge Density should maintain electric neutrality of crystal
REVIEW: The Physics of Electronics Carrier’s Concentration in extrinsic Semiconductor Mass-Action Law pn = ni2 Charge Density should maintain electric neutrality of crystal For n-type semiconductor, NA = 0; thus: For p-type semiconductor, ND = 0; thus:

5 Review: Currents in semiconductor
Jp Diffusion Current: Einstein Relationship between D and  Concentration p(x0) p(x1) x0 x1 x Dp = Diffusion Constant of Carrier

6 Review: Currents in semiconductor
Total Current: Jp Concentration p(x0) p(x1) x0 x1 x

7 Review: Graded semiconductor
Concentration x x1 x2 p(x1) p(x2) V21 p1 p2 Jp = 0; in open circuited steady state condition

8 Hamzah Afandi, Antonius Irianto dan
pn JUNCTION DIODE Hamzah Afandi, Antonius Irianto dan Betty Savitri Source: Millman, Jacob, Grabel, Arvin, Microelectronics, Mc. Graw Hill Int. Ed., 1994.

9 Open Circuited Junction
neutral neutral Semiconductors Semiconductors Holes Electrons p type n type

10 Open Circuited Junction Junction Formation
p type n type Depletion Region Space Charged Region

11 Open Circuited Junction Junction Formation
Charge Density (V) Wn -Wp p type n type Depletion Region Space Charged Region

12 Open Circuited Junction Junction Formation
Wn -Wp Field Intensity () p type n type Depletion Region Space Charged Region

13 Open Circuited Junction Junction Formation
V0 Wn -Wp V = 0 Electrostatic Potential (V) p type n type Depletion Region Space Charged Region

14 Open Circuited Junction Junction Formation
Potential Barrier of electrons(V) Wn -Wp V0 V = 0 p type n type Depletion Region Space Charged Region

15 Closed Circuited Junction Forward Biased pn Junction
p type n type Depletion Region Space Charged Region

16 Closed Circuited Junction Forward Biased pn Junction
p type n type Depletion Region Space Charged Region

17 Closed Circuited Junction Reverse Biased pn Junction
p type n type Depletion Region Space Charged Region

18 Closed Circuited Junction Reverse Biased pn Junction
p type n type Depletion Region Space Charged Region

19 Closed Circuited Junction Reverse Biased pn Junction
p type n type Depletion Region Space Charged Region

20 VOLT-AMPERE CHARACTERISTIC
 = 2 (Si)  = 1.5 (Ge) ID V -VZ VD IS (A Scale) Cut-in Offest Turn-on Breakdown

21 Diode Circuit Analysis: Load-Line Concept
+ _ VAA R VD ID ID VAA /R Solve for: VAA = 3 V R = 2 K IDQ Q VD VDQ VAA

22 CALCULATION EXAMPLES Given in class


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