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The Diode
Lecture 2
By : ENGR. SALMAN HAMEED
Last Lecture
 Atomic Structure
 Classification of matter on the basis of
semiconductor theory
 Covalent Bond
 Conduction in semiconductors
 N-type and P-type Semiconductors
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
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)
Energy Diagrams
(pn junction and Depletion Region)
At instant of junction
Formation
At equilibrium
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
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)
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
Reference
- Chapter 01 (Section 1.7 and 1.8)
“Electronic Devices” by Floyd, Seventh Edition

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The Diode_Lecture2.ppt

  • 1. The Diode Lecture 2 By : ENGR. SALMAN HAMEED
  • 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)
  • 5. Energy Diagrams (pn junction and Depletion Region) At instant of junction Formation At equilibrium
  • 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