2. Last Lecture
Atomic Structure
Classification of matter on the basis of
semiconductor theory
Covalent Bond
Conduction in semiconductors
N-type and P-type Semiconductors
3. Lecture Overview
The Diode
pn junction
Formation of Depletion Region
Energy Diagrams of the pn junction and Depletion Region
Biasing a Diode
Forward Bias
Reverse Bias
4. Diodes
N region has lots of free electrons
P region has lots of holes
At equilibrium: total number positive and negative
charges is the same (@ room temp)
At the pn junction the electrons and holes with
different charges form an electric field
In order to move electrons through the electric field
(generate current) we need some force (voltage)
– This potential difference is called barrier voltage
– When enough voltage is applied such that electrons
are moved then we are biasing the diode
– Two layers of positive and negative charges for
depletion region – the region near the pn-junction is
depleted of charge carriers)
6. Biasing Types of a Diode
Forward bias
– Bias voltage VBias > barrier voltage
VBar
– Reduction in + and – ions smaller
depletion region
– VBar Depends on material, doping,
temp, etc. (e.g., for silicon it is 0.7 V)
Reverse bias
– Essentially a condition that prevents
electrons to pass through the diode
– Very small reverse break down current
– Larger depletion region is generated
Cathode
n region
Anode
p region
Connected to the
negative side of
the battery
Connected to the
positive side of
the battery
A K
7. Biasing Types of a Diode (Forward)
Cathode
n region
Anode
p region
A K
Moving
electrons
Small dynamic resistance
VBias
n
p
Conventional
Current Flow
Conventional
Current Flow
I (Forward)
8. Very Small
Moving
Electrons:
Reverse Current)
Biasing Types of a Diode (Reverse)
Cathode
n region
Anode
p region
A K
Large resistance
VBias
n
p
Conventional
Current Flow
Holes are left
behind; large
depletion region
Instant pull of
electrons
9. Reference
- Chapter 01 (Section 1.7 and 1.8)
“Electronic Devices” by Floyd, Seventh Edition