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PN Junction Diodes
MEC
2
Contents
• PN Junction.
• Depletion Region.
• Forward Bias.
• Reverse Bias.
• Characteristic Curves.
• Zener Diodes.
• Breakdown Mechanisms.
• Zener Diode Characteristics.
• Diode Applications.
3
PN Junction
• P Type Material – Group IV semiconductor
material (Si, Ge) doped with group III
elements (B, In, Ga, etc.) – trivalent
impurity.
• N Type Material - Group IV semiconductor
material (Si, Ge) doped with group V
elements (P, As, Sb, Bi etc.) – pentavalent
impurity.
• P Type Material and N Type Material
joined together at one end.
4
PN Junction
• Doped regions meet together to form a PN
Junction.
• Permit unidirectional current flow.
• Useful in the construction of diodes.
Anode Cathode
Current flow in one
direction
5
Depletion Region
• Free electrons on the n side migrate/
diffuse across the junction to the p side.
• On the p side, free electrons are the
minority current carriers.
• Free electrons combine with holes shortly
after crossing over to the p side.
• A free electron leaves the n side and falls
into a hole on the p side, creates two ions
- a positive ion on the n side and a
negative ion on the p side.
6
Depletion Region
• Ions are immobile, electric field created.
• As the process of diffusion continues, a
barrier potential is created, diffusion of
electrons from the n side to the p side
stops.
• Electrons diffusing from the n side sense a
large negative potential on the p side that
repels them back to the n side.
7
Depletion Region
• Holes from the p side repelled back to the
p side by the positive potential on the n
side.
• Area where the positive and negative ions
are located called the depletion region.
• Word depletion used because the area
has been depleted of all charge carriers.
• Barrier potential approximately 0.7 V for Si
and 0.3 V for Ge.
8
Barrier Potential
• Barrier potential stops diffusion of current
carriers.
• Depletion region also called space charge
region.
• Cannot be measured with a voltmeter.
9
Depletion Region
Barrier Potential VB
stops carriers cross
the junction
Immobile Ions
Carriers diffuse
across the junction
due to
concentration
gradient.
10
Biasing a PN Junction
• Application of voltage/current.
• Forward Bias and Reverse Bias.
• Forward-biasing allows current to flow
easily.
• Forward Biasing reduces the width of the
potential barrier.
• Reverse biasing impedes current flow,
only leakage current flows.
• Reverse Biasing increases the width of the
potential barrier.
11
Forward Biasing
Depletion Region Narrows
V > VB
Current Limiting
Resistor
12
Forward Bias
• n material connected to the negative
terminal of the voltage source, V.
• p material is connected to the positive
terminal of the voltage source, V.
• Anode positive w.r.t cathode.
• Voltage source V repels free electrons in
the n side across the depletion zone and
into the p side.
13
Forward Bias
• On the p side, the free electron combines
with a hole.
• Electron will then travel from hole to hole
as it is attracted to the positive terminal of
the voltage source.
• For every free electron entering the n side,
one electron leaves the p side.
14
Reverse Biasing
Depletion Region Widens
Negligible current flows
through the device
15
Reverse Bias
• Negative terminal of the voltage source
connected to the p -type semiconductor
material.
• Positive terminal of the voltage source
connected to the n –type semiconductor
material.
• Charge carriers in both sections pulled
away from the junction.
16
Reverse Bias
• Free electrons on the n side pulled away
from the junction due to attraction of the
positive terminal of the voltage source.
• Holes in the p side pulled away from the
junction because of the attraction by the
negative terminal of the voltage source.
• Width of the depletion zone increases.
• Diode non-conducting, like an open
switch, ideally with infinite resistance.
17
Leakage Current
• Reverse-biased diode conducts a small
amount of current, called leakage current.
• Leakage current mainly due to minority
current carriers in both sides of the
junction.
• Minority current carriers are holes in the n
side and free electrons in the p side.
• Minority current carriers due to thermal
energy producing a few electron-hole
pairs.
18
Leakage Current
• Increase in the temperature of the diode
increases the leakage current in the diode.
• Minority current carriers move in opposite
direction to the direction provided with
forward bias.
• Also called reverse saturation current.
19
V/I Characteristics
Cut in Voltage
0.7 V for Si, 0.3 V for Ge
Diode Current rises
sharply above cut in
voltage.
Very small current
flows until VBR
Avalanche
Breakdown
Non-Linear
20
V/I Characteristics
• Forward current rises sharply above cut in
voltage.
• Current that flows prior to breakdown is
mainly due to thermally produced minority
current carriers.
• Leakage current increases mainly with
temperature, relatively independent of
changes in reverse-bias voltage.
21
V/I Characteristics
• Slight increase in reverse current with
increases in the reverse voltage due to
surface leakage current.
• Surface leakage current exists since there
are many holes on the edges of a silicon
crystal due to unfilled covalent bonds.
• Holes on the crystal edges provide a path
for a few electrons along the surfaces of
the crystal.
22
Diode Current Equation
23
Silicon Diode vs Germanium Diode
24
Avalanche Action
• Avalanche occurs when the reverse-bias
becomes excessive.
• Thermally produced free electrons on the
p side accelerated by the voltage source
to very high speeds as they move through
the diode.
• Electrons collide with valence electrons in
other orbits, sets them free.
25
Avalanche Action
• Free valence electrons accelerated to very
high speeds, dislodges more valence
electrons.
• Process is cumulative; called avalanche
effect.
• When breakdown voltage, VBR , reached,
reverse current, IR , increases sharply.
• Diodes not to be operated in breakdown
region.
• For rectifier diodes VBR > 50 V.
26
Diode Parameters
• DC Resistance of a forward biased diode
(VF - forward voltage drop and IF - the
forward current).
• Bulk resistance of a forward biased diode
(ΔV - change in diode voltage produced by
the change in diode current, ΔI).
F
F
F
V
R
I

27
Diode Approximations
• First Approximation:
- Ideal Diode Approximation.
- Forward-biased diode as a closed switch
with a voltage drop of zero volts.
- Reverse-biased diode as an open
switch with zero current.
28
First Approximation
29
Diode Approximations
• Second Approximation:
- forward-biased diode as an ideal diode
in series with a battery.
- accounts for cut in voltage.
- reverse-biased diode as an open
switch.
30
Second Approximation
31
Third Approximation
• Includes the bulk resistance, the
resistance of the p and n materials.
• Bulk resistance dependent on the doping
level and the size of the p and n materials.
• Bulk resistance causes the forward
voltage across a diode to increase slightly
with increases in the diode current.
• Resistance across the open switch is a
high leakage resistance for the reverse-
bias condition.
32
Third Approximation
D
D
D
V
r
I



Piecewise Linear Model
Slope due to rB
D
B
D
V
r
I



33
Diode Ratings
• Breakdown Voltage – voltage at which
avalanche occurs.
• Average Forward Current - maximum
allowable average current that the diode
can handle safely.
• Maximum Forward Surge Current -
maximum instantaneous current the diode
can handle safely from a single pulse (eg:
capacitor current).
34
Diode Ratings
• Maximum Reverse Current -
• Chance of diode failure if ratings
exceeded.
• Current limiting resistor in series to limit
diode current to safe values.
35
Diode Applications
• Rectifiers.
• Clippers.
• Clampers.
• Voltage Multipliers.
• For Unidirectional Current Flow.
• Surge Suppression.
36
Zener Diode
• A special diode optimized for operation in
the breakdown region.
• Connected in parallel with the load of the
power supply.
• Zener voltage remains nearly constant
despite load current variations.
• Under forward bias, zener diode acts like
an ordinary silicon diode.
37
Zener Diode
• Under reverse-bias region, a small reverse
leakage current flows until breakdown
voltage is reached.
• After breakdown voltage, reverse current
through the zener increases sharply,
reverse current called zener current.
• Breakdown voltage remains nearly
constant as the zener current increases.
• Zener diodes used as voltage regulators.
38
Zener Power Rating
• Power dissipated by the zener diode:
VZ - Zener Voltage, IZ - Zener Current.
• Both zener and avalanche breakdown
occur in zener diodes.
39
Zener Breakdown
• Reverse Voltage ≤ 6 V applied across
zener diode, narrow depletion region.
• Intense electric field of the order of 3 x 105
V/cm across the narrow depletion region.
• Electric field strong enough, to pull
electrons from the valence band to the
conduction band (free electrons) – Field
Ionisation.
• Large number of free electrons constitute
a large reverse current – zener effect.
• Occurs in heavily doped diodes.
40
Avalanche Breakdown
• In zener diodes with breakdown voltage >
6V, wider depletion region.
• Minority carriers accelerate as reverse
bias increases, their kinetic energy
increases.
• Accelerated carriers collide with stationary
atoms, impart energy to valence electrons.
• Valence electrons jump into conduction
band – free electrons and get accelerated.
41
Avalanche Breakdown
• Free electrons collide with and knock
out more valence electrons –
avalanche multiplication.
• Large reverse current flows due to
avalanche effect – impact ionisation.
• Occurs in lightly doped diodes.
• V/I characteristics not sharp in
breakdown region.
42
Zener Breakdown vs
Avalanche Breakdown
43
Zener Diode Characteristics
Sharp if zener breakdown,
more slope if avalanche
breakdown.
44
Zener Diode Applications
• Voltage Regulators.
• Clippers.
• Biased Clampers.
• Voltage Limiting.
• Voltage Overshoot Protection.
45
Zener Diode Voltage Regulators
Unloaded Loaded
IZ
IS
46
Zener Diode vs PN Junction Diode
*
* Silicon/Germanium Diode
47
Thank You

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EST 130, PN Junction Diodes

  • 2. 2 Contents • PN Junction. • Depletion Region. • Forward Bias. • Reverse Bias. • Characteristic Curves. • Zener Diodes. • Breakdown Mechanisms. • Zener Diode Characteristics. • Diode Applications.
  • 3. 3 PN Junction • P Type Material – Group IV semiconductor material (Si, Ge) doped with group III elements (B, In, Ga, etc.) – trivalent impurity. • N Type Material - Group IV semiconductor material (Si, Ge) doped with group V elements (P, As, Sb, Bi etc.) – pentavalent impurity. • P Type Material and N Type Material joined together at one end.
  • 4. 4 PN Junction • Doped regions meet together to form a PN Junction. • Permit unidirectional current flow. • Useful in the construction of diodes. Anode Cathode Current flow in one direction
  • 5. 5 Depletion Region • Free electrons on the n side migrate/ diffuse across the junction to the p side. • On the p side, free electrons are the minority current carriers. • Free electrons combine with holes shortly after crossing over to the p side. • A free electron leaves the n side and falls into a hole on the p side, creates two ions - a positive ion on the n side and a negative ion on the p side.
  • 6. 6 Depletion Region • Ions are immobile, electric field created. • As the process of diffusion continues, a barrier potential is created, diffusion of electrons from the n side to the p side stops. • Electrons diffusing from the n side sense a large negative potential on the p side that repels them back to the n side.
  • 7. 7 Depletion Region • Holes from the p side repelled back to the p side by the positive potential on the n side. • Area where the positive and negative ions are located called the depletion region. • Word depletion used because the area has been depleted of all charge carriers. • Barrier potential approximately 0.7 V for Si and 0.3 V for Ge.
  • 8. 8 Barrier Potential • Barrier potential stops diffusion of current carriers. • Depletion region also called space charge region. • Cannot be measured with a voltmeter.
  • 9. 9 Depletion Region Barrier Potential VB stops carriers cross the junction Immobile Ions Carriers diffuse across the junction due to concentration gradient.
  • 10. 10 Biasing a PN Junction • Application of voltage/current. • Forward Bias and Reverse Bias. • Forward-biasing allows current to flow easily. • Forward Biasing reduces the width of the potential barrier. • Reverse biasing impedes current flow, only leakage current flows. • Reverse Biasing increases the width of the potential barrier.
  • 11. 11 Forward Biasing Depletion Region Narrows V > VB Current Limiting Resistor
  • 12. 12 Forward Bias • n material connected to the negative terminal of the voltage source, V. • p material is connected to the positive terminal of the voltage source, V. • Anode positive w.r.t cathode. • Voltage source V repels free electrons in the n side across the depletion zone and into the p side.
  • 13. 13 Forward Bias • On the p side, the free electron combines with a hole. • Electron will then travel from hole to hole as it is attracted to the positive terminal of the voltage source. • For every free electron entering the n side, one electron leaves the p side.
  • 14. 14 Reverse Biasing Depletion Region Widens Negligible current flows through the device
  • 15. 15 Reverse Bias • Negative terminal of the voltage source connected to the p -type semiconductor material. • Positive terminal of the voltage source connected to the n –type semiconductor material. • Charge carriers in both sections pulled away from the junction.
  • 16. 16 Reverse Bias • Free electrons on the n side pulled away from the junction due to attraction of the positive terminal of the voltage source. • Holes in the p side pulled away from the junction because of the attraction by the negative terminal of the voltage source. • Width of the depletion zone increases. • Diode non-conducting, like an open switch, ideally with infinite resistance.
  • 17. 17 Leakage Current • Reverse-biased diode conducts a small amount of current, called leakage current. • Leakage current mainly due to minority current carriers in both sides of the junction. • Minority current carriers are holes in the n side and free electrons in the p side. • Minority current carriers due to thermal energy producing a few electron-hole pairs.
  • 18. 18 Leakage Current • Increase in the temperature of the diode increases the leakage current in the diode. • Minority current carriers move in opposite direction to the direction provided with forward bias. • Also called reverse saturation current.
  • 19. 19 V/I Characteristics Cut in Voltage 0.7 V for Si, 0.3 V for Ge Diode Current rises sharply above cut in voltage. Very small current flows until VBR Avalanche Breakdown Non-Linear
  • 20. 20 V/I Characteristics • Forward current rises sharply above cut in voltage. • Current that flows prior to breakdown is mainly due to thermally produced minority current carriers. • Leakage current increases mainly with temperature, relatively independent of changes in reverse-bias voltage.
  • 21. 21 V/I Characteristics • Slight increase in reverse current with increases in the reverse voltage due to surface leakage current. • Surface leakage current exists since there are many holes on the edges of a silicon crystal due to unfilled covalent bonds. • Holes on the crystal edges provide a path for a few electrons along the surfaces of the crystal.
  • 23. 23 Silicon Diode vs Germanium Diode
  • 24. 24 Avalanche Action • Avalanche occurs when the reverse-bias becomes excessive. • Thermally produced free electrons on the p side accelerated by the voltage source to very high speeds as they move through the diode. • Electrons collide with valence electrons in other orbits, sets them free.
  • 25. 25 Avalanche Action • Free valence electrons accelerated to very high speeds, dislodges more valence electrons. • Process is cumulative; called avalanche effect. • When breakdown voltage, VBR , reached, reverse current, IR , increases sharply. • Diodes not to be operated in breakdown region. • For rectifier diodes VBR > 50 V.
  • 26. 26 Diode Parameters • DC Resistance of a forward biased diode (VF - forward voltage drop and IF - the forward current). • Bulk resistance of a forward biased diode (ΔV - change in diode voltage produced by the change in diode current, ΔI). F F F V R I 
  • 27. 27 Diode Approximations • First Approximation: - Ideal Diode Approximation. - Forward-biased diode as a closed switch with a voltage drop of zero volts. - Reverse-biased diode as an open switch with zero current.
  • 29. 29 Diode Approximations • Second Approximation: - forward-biased diode as an ideal diode in series with a battery. - accounts for cut in voltage. - reverse-biased diode as an open switch.
  • 31. 31 Third Approximation • Includes the bulk resistance, the resistance of the p and n materials. • Bulk resistance dependent on the doping level and the size of the p and n materials. • Bulk resistance causes the forward voltage across a diode to increase slightly with increases in the diode current. • Resistance across the open switch is a high leakage resistance for the reverse- bias condition.
  • 32. 32 Third Approximation D D D V r I    Piecewise Linear Model Slope due to rB D B D V r I   
  • 33. 33 Diode Ratings • Breakdown Voltage – voltage at which avalanche occurs. • Average Forward Current - maximum allowable average current that the diode can handle safely. • Maximum Forward Surge Current - maximum instantaneous current the diode can handle safely from a single pulse (eg: capacitor current).
  • 34. 34 Diode Ratings • Maximum Reverse Current - • Chance of diode failure if ratings exceeded. • Current limiting resistor in series to limit diode current to safe values.
  • 35. 35 Diode Applications • Rectifiers. • Clippers. • Clampers. • Voltage Multipliers. • For Unidirectional Current Flow. • Surge Suppression.
  • 36. 36 Zener Diode • A special diode optimized for operation in the breakdown region. • Connected in parallel with the load of the power supply. • Zener voltage remains nearly constant despite load current variations. • Under forward bias, zener diode acts like an ordinary silicon diode.
  • 37. 37 Zener Diode • Under reverse-bias region, a small reverse leakage current flows until breakdown voltage is reached. • After breakdown voltage, reverse current through the zener increases sharply, reverse current called zener current. • Breakdown voltage remains nearly constant as the zener current increases. • Zener diodes used as voltage regulators.
  • 38. 38 Zener Power Rating • Power dissipated by the zener diode: VZ - Zener Voltage, IZ - Zener Current. • Both zener and avalanche breakdown occur in zener diodes.
  • 39. 39 Zener Breakdown • Reverse Voltage ≤ 6 V applied across zener diode, narrow depletion region. • Intense electric field of the order of 3 x 105 V/cm across the narrow depletion region. • Electric field strong enough, to pull electrons from the valence band to the conduction band (free electrons) – Field Ionisation. • Large number of free electrons constitute a large reverse current – zener effect. • Occurs in heavily doped diodes.
  • 40. 40 Avalanche Breakdown • In zener diodes with breakdown voltage > 6V, wider depletion region. • Minority carriers accelerate as reverse bias increases, their kinetic energy increases. • Accelerated carriers collide with stationary atoms, impart energy to valence electrons. • Valence electrons jump into conduction band – free electrons and get accelerated.
  • 41. 41 Avalanche Breakdown • Free electrons collide with and knock out more valence electrons – avalanche multiplication. • Large reverse current flows due to avalanche effect – impact ionisation. • Occurs in lightly doped diodes. • V/I characteristics not sharp in breakdown region.
  • 43. 43 Zener Diode Characteristics Sharp if zener breakdown, more slope if avalanche breakdown.
  • 44. 44 Zener Diode Applications • Voltage Regulators. • Clippers. • Biased Clampers. • Voltage Limiting. • Voltage Overshoot Protection.
  • 45. 45 Zener Diode Voltage Regulators Unloaded Loaded IZ IS
  • 46. 46 Zener Diode vs PN Junction Diode * * Silicon/Germanium Diode