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ELECTRONIC SYSTEM AND
PCB DESIGN(21ECC101J )
Unit-1
DR. AARTI SHARMA
ASSISTANT PROFESSOR
DEPARTMENT OF ECE
SRM IST, DELHI NCR CAMPUS
1
Course outcome of Unit-1
 At the end of this unit student will get to know about the
basics of semiconductors and semiconductor devices.
2
Contents
 Classifications of Semiconductor
 Doping in Semiconductors
 Conductivity of semiconductors
 Energy Distribution and fermi level
 Carrier Concentration in intrinsic semiconductor and
Mass-Action Law
 Drift and Diffusion Current
 Einstein Relationship for semiconductors
3
1. Semiconductors 4
2. Doping in Semiconductors 5
Intrinsic semiconductors
 An intrinsic semiconductor is one which is made of the semiconductor
material in its extremely pure form.
Examples : Si, Ge
 The energy gap is so small that even at ordinary room temperature; there
are many electrons which possess sufficient energy to jump across the
small energy gap between the valence and the conduction bands.
 Alternatively, an intrinsic semiconductor may be defined as one in which
the number of conduction electrons is equal to the number of holes.
6
Fermi Energy and Fermi Level
 Fermi Energy
It is the maximum energy possessed by free electron at
absolute zero temperature.
 Fermi level
It is the highest energy state occupied by free electron at
absolute zero temperature.
7
Fermi Level 8
Conductivity of Semiconductor 9
Where σ is the conductivity of the semiconductor.
Fermi Dirac Function
 Fermi Dirac Distribution is the probability distribution function which states
the probability of finding an electron in the given energy level.
10
Explanation 11
Carrier Concentration in Intrinsic semiconductor 12
 In Intrinsic semiconductor when the valence electron broke covalent bond and
jump into conduction band two types of charge carriers are generated. They are
electrons and holes.
Intrinsic carrier concentration
 The number of electron per unit volume in conduction band or number of holes
per unit volume in valence band is called intrinsic carrier concentration.
Mass Action Law

13
Drift Current 14
 The current flow in semiconductor under the influence of electric field is
called drift current.
Diffusion Current
 The current flow in semiconductor from region of higher
concentration to the lower concentration is called diffusion
current.
15
Einstein Relationship
 The equation which relates the mobility and the diffusion constant is
known as Einstein relationship.
16
P-N Junction Diode 17
18
19
20
21
BJT Configurations 22
MOSFET 23
D-MOSFET 24
Enhancement type MOSFET 25
Double Gate MOSFET 26
Construction of Dual Gate MOSFET 27
Working of Dual Gate MOSFET 28
V-I Characteristic of Dual Gate MOSFET 29
Advantages of Dual Gate MOSFET
1) Reduced channel and gate leakage current at off state which
saves power.
2) Separate gate control on voltage saves power and chip area.
30
Challenges in Dual Gate MOSFET
1) Identically sized gates
2) Self alignment of source and drain to both gates
3) Alignment of both gates to each other
4) Connecting two gates with low resistance path
31
Applications of Dual Gate MOSFET
1) Mixers
2) Demodulators
3) Cascade amplifiers
4) Radio Frequency (RF) amplifier
5) Automatic Gain Control (AGC) amplifier
32
Fin FET
.
33
MOSFET Scaling
.
34
Issues in Nano MOSFETs 35
Issues in Nano MOSFETs 36
Issues in Nano MOSFETs 37
38
Planar MOSFET VS. Fin FET 39
Structure of Fin FET
.
40
Classification of Fin FET 41
Short Gate (SG) and Insulated Gate (IG)
FET
42
Short Gate (SG) vs. Insulated Gate (IG)
FET
43
Short Gate (SG) and Insulated Gate (IG)
FET
44
45
Bulk Fin FET vs. SOI Fin FET 46
47
48
49
50
51
Fabrication of Fin (Bulk Fin) 52
Fabrication of Fin (Bulk Fin) 53
54
55
56
57
Future of Fin FET 58

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