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Lecture 5.0 Properties of Semiconductors. Importance to Silicon Chips Size of devices –Doping thickness/size –Depletion Zone Size –Electron Tunneling.

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Presentation on theme: "Lecture 5.0 Properties of Semiconductors. Importance to Silicon Chips Size of devices –Doping thickness/size –Depletion Zone Size –Electron Tunneling."— Presentation transcript:

1 Lecture 5.0 Properties of Semiconductors

2 Importance to Silicon Chips Size of devices –Doping thickness/size –Depletion Zone Size –Electron Tunneling dimension Chip Cooling- Device Density –Heat Capacity –Thermal Conductivity

3 Band theory of Semiconductors Forbidden Zone – ENERGY GAP Valence Band Conduction Band

4 Silicon Band Structure - [Ne]3s 2 3p 2

5 Fermi-Dirac Probability Distribution for electron energy, E Probability, F(E)= (e {[E-E f ]/k B T} +1) -1 –E f is the Fermi Energy

6 Number of Occupied States Fermi-Dirac Density of States T>0

7 Difference between Semiconductors and Insulators MaterialE g (eV) InSb0.18 InAs0.36 Ge0.67 Si1.12 GaAs1.43 SiC2.3 ZnS3.6 NiO4.2 Al 2 O 3 8 k B T =0.0257 eV at 298˚K

8 Probability of electrons in Conduction Band Lowest Energy in CB E-E f  E g /2 Probability in CB F(E)= (exp{[E-E f ]/k B T} +1) -1 ) = (exp{E g /2k B T} +1) -1  exp{-E g /2k B T} for E g >1 eV @ 298K k B T =0.0257 eV at 298˚K

9 Variation of Conductivity with T  =d  /dT

10 Intrinsic Conductivity of Semiconductor Charge Carriers –Electrons –Holes  = n e e  e + n h e  h # electrons = # holes –   n e e (  e +  h ) –n e  C exp{-E g /2k B T} n e =2(2  m* e k B T/h 2 ) 3/2 exp(-E g /(2k B T)) E f =E g /2+3/4k B T ln(m* h /m* e )

11 Mobilities

12 Semiconductor Photoelectric Effect Light Absorption/Light Emission (photodetector)/(photo diode laser) Absorption max =hc/E g

13 Light Emitting Diode

14 Photodiode Laser Color depends on band gap, E g =hc/E g Pb 0.37 0.27 0.33 IR detectors E g >3.0 transparent

15 Diode Laser

16 Extrinsic Conductivity of Semiconductor Donor Doping Acceptor Doping n-type p-type p= 2(2  m* h k B T/h 2 ) 3/2 exp(-E f /k B T) Law of Mass Action, N i p i =n d p d or =n n d n N=n d +n i

17 Extrinsic Conductivity of Semiconductor Donor Doping Acceptor Doping

18 Electron Density Dopant Concentration effects Electron Density Electrical Conductivity

19 Conductivity Intrinsic Range –Exponential with T Extrinsic Range –Promoted to CB   –Decreasing ,  –Joins Intrinsic   Majority/minority Carriers  = n e e  e + n h e  h

20 Majority/minority Carriers Conductivity  = n e e  e + n h e  h n-typen e >>n h Low number of holes due to recombination. Law of Mass Action –N i p i =n d p d –(For p-type N i p i =n n d n )

21 Extrinsic Conductivity of Semiconductor Donor Doping Acceptor Doping n-type p-type E d = -m* e e 4 /(8 (  o ) 2 h 2 ) E f =E g -E d /2 E f =E g +E a /2

22 Effective Mass Holes Electrons

23 Wafer Sales Following PRIME GRADE Si wafers are all single-side polish $14.50 each for 25 wafers each $11.00 for 50 or more (we can double side polish) –4" P 3.0-6.6 ohm-cm –4" N 4.0-6.0 ohm-cm –4" P 7.0-21.6 ohm-cm –4" P 12.0-16.0 ohm-cm –4" P 3.0-5.0 ohm-cm http://www.collegewafer.com/

24 GaP Wafer 2" Undoped (100) $180.00 each 2" S doped (111) $180.00 each

25 C&ENews 1/6/03


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