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Presentation
On Tunnel diode
Submitted To :
Farzana Rahman Mishu
Sr. Lecturer
Department of CSE
University of Development Alternative
Date of Submission:
29/08/2015
Submitted By:
Md. Sohel Sarker
UODA
Presented By
Sohel Sarker
011-121-010
Fatema Tuj
Zohra
011-141-021
Safia Hussain
011-141-022
Introduction
Invented by Dr. Leo Esaki
in 1958.
Also called Esaki diode.
Basically, it is heavily
doped PN- junction.
These diodes are
fabricated from
germanium, gallium
arsenide & Gallium
Antimonide.
Description
Tunnel diode is a semi-conductor
with a special characteristic of
negative resistance.
By negative resistance, we mean that
when voltage is increased, the
current through it decreases.
Highly doped PN- junction. Doping
density of about 1000 times greater
than ordinary junction diode.
Construction
Heavy Doping Effects:
• Reduces the width of depletion layer to about 0.00001
mm.
• Produces negative resistance section in characteristics
graph of diode.
• Reduces the reverse breakdown voltage to a small
value approaches to zero.
• Small forbidden gaps in tunnel diode.
• Allows conduction for all reverse voltages.
Basic principle of
operation:
The operation depends upon quantum
mechanics principle known as “tunneling”.
The movement of valence electrons from
valence energy band to conduction band with no
applied forward voltage is called “tunneling”.
Intrinsic voltage barrier is reduced which
enhanced tunneling.
Enhanced tunneling causes effective conductivity.
Working
At first voltage begin to increase,
Electrons tunnel through pn junction.
Electron and holes states become aligned.
Voltage increases further:
States become misaligned.
Current drops.
Shows negative resistance (V increase, I decrease).
As voltage increase yet further:
The diode behave as normal diode.
The electrons no longer tunnel through barrier.
Forward Bias operation:
Working(contd.)
The electrons in valence band
of p-side tunnel directly
towards the empty states
present in the conduction band
of n-side.
Thus, creating large tunneling
current which increases with
application of reverse voltage.
When used in reverse direction,
they are called as Back Diodes.
I/V Characteristics
As forward bias is applied,
significant I is produced.
After continuous increase of V, the
current achieves its minimum
value called as Valley Current.
After further increase in V, current
start increasing as ordinary diode.
Applications:
It is used as an ultra- high speed switch due to tunneling (which essentially takes
place at speed of light). It has switching time of nanoseconds or picoseconds.
Used as logic memory storage device.
In satellite communication equipment, they are widely used.
Due to its feature of –ive resistance, it is used in relaxation oscillator circuits.
Applications(contd.):
Tunnel diodes are
resistant to the
effects of magnetic
fields, high
temperature and
radioactivity. That’s
why these can be
used in modern
military equipments
- NMR machines.
Due to low power
requirement, they
are used in FM
receivers.
Tunnel diode

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Tunnel diode

  • 1. Presentation On Tunnel diode Submitted To : Farzana Rahman Mishu Sr. Lecturer Department of CSE University of Development Alternative Date of Submission: 29/08/2015 Submitted By: Md. Sohel Sarker UODA
  • 2. Presented By Sohel Sarker 011-121-010 Fatema Tuj Zohra 011-141-021 Safia Hussain 011-141-022
  • 3. Introduction Invented by Dr. Leo Esaki in 1958. Also called Esaki diode. Basically, it is heavily doped PN- junction. These diodes are fabricated from germanium, gallium arsenide & Gallium Antimonide.
  • 4. Description Tunnel diode is a semi-conductor with a special characteristic of negative resistance. By negative resistance, we mean that when voltage is increased, the current through it decreases. Highly doped PN- junction. Doping density of about 1000 times greater than ordinary junction diode.
  • 5. Construction Heavy Doping Effects: • Reduces the width of depletion layer to about 0.00001 mm. • Produces negative resistance section in characteristics graph of diode. • Reduces the reverse breakdown voltage to a small value approaches to zero. • Small forbidden gaps in tunnel diode. • Allows conduction for all reverse voltages.
  • 6. Basic principle of operation: The operation depends upon quantum mechanics principle known as “tunneling”. The movement of valence electrons from valence energy band to conduction band with no applied forward voltage is called “tunneling”. Intrinsic voltage barrier is reduced which enhanced tunneling. Enhanced tunneling causes effective conductivity.
  • 7. Working At first voltage begin to increase, Electrons tunnel through pn junction. Electron and holes states become aligned. Voltage increases further: States become misaligned. Current drops. Shows negative resistance (V increase, I decrease). As voltage increase yet further: The diode behave as normal diode. The electrons no longer tunnel through barrier. Forward Bias operation:
  • 8. Working(contd.) The electrons in valence band of p-side tunnel directly towards the empty states present in the conduction band of n-side. Thus, creating large tunneling current which increases with application of reverse voltage. When used in reverse direction, they are called as Back Diodes.
  • 9. I/V Characteristics As forward bias is applied, significant I is produced. After continuous increase of V, the current achieves its minimum value called as Valley Current. After further increase in V, current start increasing as ordinary diode.
  • 10. Applications: It is used as an ultra- high speed switch due to tunneling (which essentially takes place at speed of light). It has switching time of nanoseconds or picoseconds. Used as logic memory storage device. In satellite communication equipment, they are widely used. Due to its feature of –ive resistance, it is used in relaxation oscillator circuits.
  • 11. Applications(contd.): Tunnel diodes are resistant to the effects of magnetic fields, high temperature and radioactivity. That’s why these can be used in modern military equipments - NMR machines. Due to low power requirement, they are used in FM receivers.