Lecture 5 0 Properties of Semiconductors Importance to

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Lecture 5. 0 Properties of Semiconductors

Lecture 5. 0 Properties of Semiconductors

Importance to Silicon Chips l Size of devices – Doping thickness/size – Depletion Zone

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

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

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

Silicon Band Structure - [Ne]3 s 23 p 2

Silicon Band Structure - [Ne]3 s 23 p 2

Fermi-Dirac Probability Distribution for electron energy, E l. Probability, F(E)= (e{[E-Ef]/k. BT}+1)-1 –Ef is

Fermi-Dirac Probability Distribution for electron energy, E l. Probability, F(E)= (e{[E-Ef]/k. BT}+1)-1 –Ef is the Fermi Energy

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

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

Difference between Semiconductors and Insulators Material Eg(e. V) In. Sb 0. 18 In. As

Difference between Semiconductors and Insulators Material Eg(e. V) In. Sb 0. 18 In. As 0. 36 Ge 0. 67 Si 1. 12 Ga. As 1. 43 Si. C 2. 3 Zn. S 3. 6 Ni. O 4. 2 Al 2 O 3 k. BT =0. 0257 e. V at 298˚K 8 Eg>3. 0 e. V transparent

Probability of electrons in Conduction Band Lowest Energy in CB l E-Ef Eg/2 l

Probability of electrons in Conduction Band Lowest Energy in CB l E-Ef Eg/2 l Probability in CB l F(E)= (exp{[E-Ef]/k. BT} +1)-1 ) l = (exp{Eg/2 k. BT} +1)-1 l exp{-Eg/2 k. BT} for Eg>1 e. V @ 298 K l k. BT =0. 0257 e. V at 298˚K

Variation of Conductivity with T =d /d. T

Variation of Conductivity with T =d /d. T

Intrinsic Conductivity of Semiconductor l Charge Carriers – Electrons – Holes l = n

Intrinsic Conductivity of Semiconductor l Charge Carriers – Electrons – Holes l = n e e e + n h e h l # electrons = # holes – ne e ( e+ h) – ne C exp{-Eg/2 k. BT} ne=2(2 m*e k. BT/h 2)3/2 exp(-Eg /(2 k. BT)) Ef=Eg/2+3/4 k. BT ln(m*h/m*e)

Mobilities

Mobilities

Semiconductor Photoelectric Effect l Light Absorption/Light Emission (photodetector)/(photo diode laser) l Absorption max =hc/Eg

Semiconductor Photoelectric Effect l Light Absorption/Light Emission (photodetector)/(photo diode laser) l Absorption max =hc/Eg

Light Emitting Diode

Light Emitting Diode

Photodiode Laser l Color depends on band gap, Eg l =hc/Eg Eg>3. 0 transparent

Photodiode Laser l Color depends on band gap, Eg l =hc/Eg Eg>3. 0 transparent Pb 0. 37 0. 27 0. 33 IR detectors

Diode Laser

Diode Laser

Extrinsic Conductivity of Semiconductor l Donor l n-type N=nd+ni Doping Acceptor Doping p-type p=

Extrinsic Conductivity of Semiconductor l Donor l n-type N=nd+ni Doping Acceptor Doping p-type p= 2(2 m*h k. BT/h 2)3/2 exp(-Ef/k. BT) Law of Mass Action, Nipi=ndpd or =nndn

Extrinsic Conductivity of Semiconductor l Donor Doping Acceptor Doping

Extrinsic Conductivity of Semiconductor l Donor Doping Acceptor Doping

Electron Density l Dopant Concentration effects l Electron Density l Electrical Conductivity

Electron Density l Dopant Concentration effects l Electron Density l Electrical Conductivity

Conductivity l Intrinsic Range – Exponential with T l Extrinsic Range – Promoted to

Conductivity l Intrinsic Range – Exponential with T l Extrinsic Range – Promoted to CB • – Decreasing , – Joins Intrinsic l Majority/minority Carriers l = ne e e + nh e h

Majority/minority Carriers l Conductivity l = n e e e + n h e

Majority/minority Carriers l Conductivity l = n e e e + n h e h l n-type ne>>nh l Low number of holes due to recombination. l Law of Mass Action – Nipi=ndpd – (For p-type Nipi =nndn )

Extrinsic Conductivity of Semiconductor l Donor Doping l n-type Ed = -m*e e 4/(8

Extrinsic Conductivity of Semiconductor l Donor Doping l n-type Ed = -m*e e 4/(8 ( o)2 h 2) Ef=Eg-Ed/2 Acceptor Doping p-type Ef=Eg+Ea/2

Effective Mass l Holes l Electrons

Effective Mass l Holes l Electrons

Wafer Sales l Following PRIME GRADE Si wafers are all single-side polish $14. 50

Wafer Sales l 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) – – – l 4" P<111> 4" N<100> 4" P<111> 4" P<100> 4" P<111> 3. 0 -6. 6 ohm-cm 4. 0 -6. 0 ohm-cm 7. 0 -21. 6 ohm-cm 12. 0 -16. 0 ohm-cm 3. 0 -5. 0 ohm-cm http: //www. collegewafer. com/

Ga. P Wafer 2" Undoped (100) $180. 00 each 2" S doped (111) $180.

Ga. P Wafer 2" Undoped (100) $180. 00 each 2" S doped (111) $180. 00 each

C&ENews 1/6/03

C&ENews 1/6/03