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Electrical Engineering 2

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Presentation on theme: "Electrical Engineering 2"— Presentation transcript:

1 Electrical Engineering 2
Lecture 13 Microelectronics 2 Dr. Peter Ewen (Room G08, SMC; - pjse)

2 The Abrupt Junction Diffusion Implantation Abrupt junction model NA
Dopant concentration NA or ND Dopant concentration NA or ND p n p n xj xj ND ND Depth into wafer, x Depth into wafer, x ABRUPT JUNCTION LINEARLY-GRADED JUNCTION

3 c = e(p – n + ND – NA)  = (p – n + ND – NA) junction p-type n-type -
-ve +ve The charges in the depletion region are those on the carriers and on the charged impurity ions fixed in the lattice. E depletion region Taking the sign of the charges into account: c = e(p – n + ND – NA) dE e dx   = (p – n + ND – NA) For simplicity take n = 0 & p = 0 – the depletion approximation

4 Depletion region - + - - + - + + + - - - + + - + - + - + + - + + + + - - - + - + - - - + - - + + - + + - p-type lp x= ln n-type junction Charge density variation through a pn junction density, c Charge eND Distance, x -eNA Fig. 76.2

5 To find the Electric Field
For the p-type side we have: Poisson’s equation on p-type side Since NA is constant (abrupt junction) Since E = 0 outside the depletion region, i.e. at x  Ip Similarly, for the n-type side:

6 To find the Potential The electric field, E, is defined by:
For the p-type side we have: If we take the zero of potential to be at x = 0 then C' = 0.

7 - - - - - - - - - - - VB + + - + + + - - + + + - + + + - + + + + - - -
eND p-type lp x= ln n-type density, c Charge Distance, x -eNA Electric field, E E Distance, x Ep En Emax Vn VB Potential, V Vp Distance, x

8 MOS Transistor – Basic Structure
Gate Source Drain n-channel device +Vg Metal Oxide Semiconductor SiO2 n+ n+ Channel p-type substrate Fig. 80

9 LECTURE 13 Operation of the MOS transistor – gate-controlled surface effects MOS fabrication – enhancement and depletion devices MOS Pinch-off

10 Gate-Controlled Surface effects Fig. 81 - - drain SiO2 n+ metal - -
p-type substrate n-channel device (enhancement) holes + source n+ - acceptor ions - electrons −ve voltage on gate +ve voltage on gate Charge QG Channel forms when the +ve voltage on the gate is greater than VT (threshold voltage) QA (A ≡ Accumulation) QA = -QG Distance “Inversion” occurs QD (D ≡ Depletion) QD = -QG QC + QG QC (C ≡ Channel)

11 Gate-Controlled Surface effects Fig. 82 drain SiO2 p+ metal gate
p-channel device n-type substrate Fig. 82 source p+ -ve voltage on gate with magnitude greater than VT Charge QC QD Distance QG

12 MOS Threshold Voltage An n-channel polysilicon gate MOS transistor has the following features: oxide thickness tox = 0.1 m channel width W = 18 m channel length L = 6 m substrate doping NA = 5x1022 m-3 oxide relative permittivity ox = 4 EF − EV for substrate = eV Eg = 1.1 eV for Si Determine the gate capacitance, Cg. If the depth of the depletion region at VG = VT is 0.14 m, how much of VT goes to creating QD?

13 Determine the gate capacitance, Cg.
oxide thickness tox = 0.1 m channel width W = 18 m channel length L = 6 m substrate doping NA = 5x1022 m-3 oxide relative permittivity ox = 4 EF − EV for substrate = eV Eg = 1.1 eV for Si 1. MOS threshold voltage Determine the gate capacitance, Cg. L SiO2 SiO2 SiO2 W Gate conductor (metal) insulator (oxide) conductor (silicon) Source Source Source Drain Drain Drain n+ n+ n+ n+ n+ n+ tox

14 (b) If the depth of the depletion region at
VG = VT is 0.14 m, how much of VT goes to creating QD? oxide thickness tox = 0.1 m channel width W = 18 m channel length L = 6 m substrate doping NA = 5x1022 m-3 oxide relative permittivity ox = 4 EF − EV for substrate = eV Eg = 1.1 eV for Si Gate region of n-channel MOS VT +ve Gate SiO2 _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ inversion layer of electrons _ _ depletion region ionised acceptor atoms p-type substrate

15 Gate region of n-channel MOS
The part of VT that goes into creating the depletion charge QD is therefore depth of depletion region – 0.14 m oxide thickness tox = 0.1 m channel width W = 18 m channel length L = 6 m substrate doping NA = 5x1022 m-3 oxide relative permittivity ox = 4 EF − EV for substrate = eV Eg = 1.1 eV for Si Gate region of n-channel MOS Gate VT +ve SiO2 _ Depth _ _ _ _ _ W L p-type substrate

16 (c) If effective inversion occurs when the channel is as n-type as the wafer is p-type, determine an approximate value for VT. For effective inversion EF must be 0.175eV below EC in the n-type channel, i.e. the band diagram must move down by: (1.1 – 20.175)eV = 0.75eV. p-type substrate C.B. V.B. EC EF EV 1.1eV 0.175eV n-channel C.B. V.B. EC EV 1.1eV n-channel C.B. EC EF EV (1.1 – 20.175)eV = 0.75eV 1.1eV 0.175eV V.B.

17 What voltage must be applied to the gate to achieve this?

18 MOS Fabrication Fig. 83 n-channel enhancement device donor diffusion
Polysilicon Gate polycrystalline Si (“polysilicon”) Source Drain Al Al SiO2 n+ n+ “self-aligned” gate n+ → “+” indicates heavy doping p-type substrate (wafer) NA ~ 1020 m-3

19 Gate Contact Fig. 84 Gate contact made here n-channel device Source
Drain SiO2 n+ n+ Fig. 84

20 MOS Fabrication n-channel depletion device Polysilicon Gate
Source Drain Al Al SiO2 n+ n+ Implanted channel p-type substrate (wafer) NA ~ 1020 m-3

21 Same considerations apply to p-channel devices.
n-channel enhancement device n-channel depletion device Polysilicon Gate Polysilicon Gate Source Drain Source Drain Al Al Al Al n+ n+ n+ n+ Implanted channel IDS IDS VT VGS VT VGS Same considerations apply to p-channel devices.

22 Vox ≥ VT everywhere between source and drain.
MOS Pinch-off Fig. 85 n-channel enhancement device +8V +7.5V +7V 0V VT = 1 V gate source drain SiO2 n+ -eE→ n+ inversion layer depletion region p-type substrate Vox ≥ VT everywhere between source and drain. Vox drops below VT at drain end – channel becomes interrupted or “pinched off”

23 VGD = VT  VGS – VDS = VT  VDS = VGS – VT
Condition for pinch-off Fig. 86 n-channel enhancement device +8V gate 7.5V +7V 0V VT = 1 V VGS VGD source drain SiO2 n+ n+ VDS Vox is smallest at the drain end of the gate, hence pinch-off first occurs when VGD = VT G VGD VGD = VT  VGS – VDS = VT  VDS = VGS – VT D VGS VDS S Pinch-off first appears when: VDS = VGS – VT

24 Condition for pinch-off – all devices
n-channel device p-channel device The channel will be pinched-off if the voltage difference across the oxide layer at the drain end of the channel (i.e. VGD) is less than VT The channel will be pinched-off if the voltage difference across the oxide layer at the drain end of the channel (i.e. VGD) is greater than VT gate gate drain drain VGD VGD VT +ve VT -ve n+ n+ n+ n+ VGD = VGS – VDS G VGD > VT VGS – VDS > VT  VDS < VGS – VT VGD < VT VGS – VDS < VT  VDS > VGS – VT D VGS VDS S

25 Conditions for pinch-off – all devices
The channel will be pinched-off if: n-channel enhancement device VDS > VGS – VT n-channel depletion device p-channel enhancement device VDS < VGS – VT p-channel depletion device n-channel enhancement device n-channel depletion device p-channel enhancement device p-channel depletion device VDS +ve -ve VGS +ve or -ve -ve or +ve VT

26 source gate drain n+ source gate drain n+ ID VDS>VGS-VT VDS=VGS-VT VDS Effect of pinch-off on the current through the device

27 2. Pinch-off The terminal voltages for an n-channel enhancement MOS transistor with VT = 1V are given below. Is the channel pinched off? VG = 5V VD = 4.5V VS = 3V

28 To see if the channel is pinched off we need to compareVDS with
VGS – VT . Device is n-channel so if VDS > VGS – VT the channel is pinched off VDS < VGS – VT the channel is not pinched off VDS is the voltage on the drain with respect to the source: VDS = VD – VS = 4.5 – 3 = 1.5V VGS is the voltage on the gate with respect to the source: VGS = VG – VS = 5 – 3 = 2V VGS – VT = 1, hence VDS > VGS – VT and so the channel is pinched off. +5V 4.5V +7V 3V VT = 1 V VGS gate source drain n+ n+ VDS

29 Summary MOS OPERATION n-channel device:
SiO2 n+ metal n-channel device (enhancement) gate p-type substrate MOS OPERATION n-channel device: VG ≤ 0 – no conduction between source and drain possible because one of the two pn junctions around source and drain is reverse biased. 0 < VG < VT – mobile holes repelled from surface below gate. (VT is the Threshold Voltage.) VG > VT – electrons attracted to surface below gate, surface inverted to become n-type, conduction between source and drain. source n+

30 MOS FABRICATION n-channel device: Lightly-doped p-type wafer Grow thin SiO2 layer for gate insulation Deposit polycrystalline silicon for gate electrode Diffuse/implant n-type dopant for source and drain (n+) Make metal contacts – (gate contact offset)

31 ENHANCEMENT AND DEPLETION MOSFET’s
Enhancement device – no channel between source and drain for VGS = 0 Depletion device – channel deliberately created between source and drain during fabrication. Hence there are 4 MOSFET types: n-channel enhancement n-channel depletion p-channel enhancement p-channel depletion

32 MOS PINCH-OFF Channel between source and drain becomes pinched off (i.e. interrupted) when: VDS ≥ VGS – VT ID VDS VDS=VGS-VT VDS>VGS-VT


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