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Basic Electronics
Lecture#5
Semiconductor Material/
Devices and PN-
Junction
By: sarmad baloch
Class of BS.IT, ISP
An Atom
This model was proposed by
Niels Bohr in 1915.
• electrons circle the nucleus.
• nucleus made of:
i) +protons
ii) Neutral:neutron
Bohr model of an atom
What is Conductor?
•An element that can easily pass current
•We can also say that an atom that can easily lose an electron from
its outermost shell.
•Conductors have loosely bound electrons in their outer shell
•These electrons require a small amount of energy to free them for
conduction
•The force on each electron is enough to free it from its orbit and it
can jump from atom to atom – the conductor conducts
•Conductors have a low resistance.
Conductor
Slide 4
•Insulators have tightly bound electrons in their outer shell
•These electrons require a very large amount of energy to free
them for conduction
•The force on each electron is not enough to free it from its
orbit and the insulator does not conduct
•Insulators are said to have a high resistivity / resistance
Insulator
Semiconductor
•Definition: Semiconductors are those materials that have
a resistance between that of conductors and insulators
•Their electrons are not free to move but a little energy will
free them for conduction
•The two most common semiconductors are silicon and
germanium
Conductor, Insulator, Semiconductor
Energy Band
Energy Bands
•Energy gap-the difference between the energy levels of any two orbital shells
•Band-another name for an orbital shell (valence shell=valence band)
•Conduction band –the band outside the valence shell
Silicon Atom and Covalent Bond
•Silicon has a valency
of 4 i.e. 4 electrons in
its outer shell
•Each silicon atom
shares its 4 outer
electrons with 4
neighbouring atoms
•These shared
electrons – bonds – are
shown as horizontal
and vertical lines
between the atoms
Slide 8
This picture shows the
shared electrons
Heating Silicon
•We have seen that, in
silicon, heat releases
electrons from their
bond.
•This creates electron-
hole pairs which are then
available for conduction
Slide 9
Heating Silicon
•If more heat is applies the
process continues…
Slide 10
•More heat…
•More current…
•Less resistance…
•The silicon is acting as a
thermistor
Its resistance decreases with
temperature
Forming P-Type and
N-Type material Using
Silicon Doping
Intrinsic And Extrinsic
Semiconductor
•Intrinsic Semiconductor: A semiconductor in its pure from is called
Intrinsic Semiconductor. It is undoped.
• Extrinsic Semiconductor: A semiconductor in its impure form or
semi conductor which is doped is called is called extrinsic
Semiconductor.
Doping Of An Intrinsic Semiconductor
• Definition: Doping is a process of adding impurity to a
pure semiconductor is called the doping of a
semiconductor.
•When semiconductor is doped, P-Type or N-Type
Semiconductor material is form.
•N-Type semiconductor material have majority of
electrons.
•P-Type semiconductor material have majority of holes.
Forming N-Type
Semiconductor
material Using Silicon
Doping
N-Type Semiconductor Material
Slide 15
•Phosphorus is
number 15 in the
periodic table
•It has 15 protons and
15 electrons – 5 of
these electrons are in
its outer shell
N-Type Semiconductor Material
•Suppose we
remove a silicon
atom from the
crystal lattice.
•We replace it with
a phosphorus atom
•We now have an
electron that is not
bonded – it is thus
free for conduction
Slide 16
N-Type Semiconductor Material
•Let’s remove another
silicon atom and replace it
with a phosphorus atom.
Slide 17
•As more electrons are
available for
conduction we have
increased the
conductivity of the
material
•If we now apply a potential difference across the
silicon
•Phosphorus is called the
dopant
Extrinsic Conduction In N-Type
Semiconductor Material
•A current will
flow
•Note: The
negative
electrons move
towards the
positive terminal
Slide 18
N-Type Silicon Material
 This type of silicon is called n-type
 This is because the majority charge carriers are negative
electrons
 A small number of minority charge carriers – holes – will
exist due to electrons-hole pairs being created in the silicon
atoms due to heat
 The silicon is still electrically neutral as the number of
protons is equal to the number of electrons
Slide 19
Forming P-Type
Semiconductor
material Using Silicon
Doping
How P-Type Material Is Forming Using
Boron Atom
Slide 21
•Boron is
number 5 in the
periodic table
•It has 5 protons and
5 electrons – 3 of
these electrons are
in its outer shell
Doping – Making p-type Silicon
•As before, we
remove a silicon
atom from the
crystal lattice
•This time we
replace it with a
boron atom
•Notice we have a
hole in a bond – this
hole is thus free for
conduction Slide 22
Doping – Making p-type Silicon
•Let’s remove another
silicon atom. and replace it
with another boron atom
•As more holes are available
for conduction we have
increased the conductivity of
the material
Slide 23
•If we now apply a potential difference across the
silicon.
•Boron is the dopant in
this case.
Extrinsic Conduction – p-type silicon
A current will
flow – this time
carried by
positive holes
Note:
The positive
holes move
towards the
negative terminal
Slide 24
Holes & Hole Current
+ + ++
+
+
+
+
+
+
+
+
+
Hole Movement
Electron Movement
P-type Silicon
 This type of silicon is called p-type
 This is because the majority charge carriers are positive
holes
 A small number of minority charge carriers – electrons –
will exist due to electrons-hole pairs being created in the
silicon atoms due to heat
 The silicon is still electrically neutral as the number of
protons is equal to the number of electrons
Donor And Acceptor Impurity Atom
• Acceptor Dopant: an acceptor is a dopant atom that when
added to a semiconductor can form a p-type region.
•Donor Dopant: a donor is a dopant atom that, when added
to a semiconductor, can form an n-type region.
•Trivalent Impurity: P-type material is formed. Boron is
trivalent impurity
•Pentavalent Impurity: N-Type Material is formed.
Phosphorus is pentavalent impurity.
Semiconductor materials and pn junction by sarmad baloch

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Semiconductor materials and pn junction by sarmad baloch

  • 1. Basic Electronics Lecture#5 Semiconductor Material/ Devices and PN- Junction By: sarmad baloch Class of BS.IT, ISP
  • 2. An Atom This model was proposed by Niels Bohr in 1915. • electrons circle the nucleus. • nucleus made of: i) +protons ii) Neutral:neutron Bohr model of an atom
  • 3. What is Conductor? •An element that can easily pass current •We can also say that an atom that can easily lose an electron from its outermost shell. •Conductors have loosely bound electrons in their outer shell •These electrons require a small amount of energy to free them for conduction •The force on each electron is enough to free it from its orbit and it can jump from atom to atom – the conductor conducts •Conductors have a low resistance.
  • 5. •Insulators have tightly bound electrons in their outer shell •These electrons require a very large amount of energy to free them for conduction •The force on each electron is not enough to free it from its orbit and the insulator does not conduct •Insulators are said to have a high resistivity / resistance Insulator
  • 6. Semiconductor •Definition: Semiconductors are those materials that have a resistance between that of conductors and insulators •Their electrons are not free to move but a little energy will free them for conduction •The two most common semiconductors are silicon and germanium
  • 7. Conductor, Insulator, Semiconductor Energy Band Energy Bands •Energy gap-the difference between the energy levels of any two orbital shells •Band-another name for an orbital shell (valence shell=valence band) •Conduction band –the band outside the valence shell
  • 8. Silicon Atom and Covalent Bond •Silicon has a valency of 4 i.e. 4 electrons in its outer shell •Each silicon atom shares its 4 outer electrons with 4 neighbouring atoms •These shared electrons – bonds – are shown as horizontal and vertical lines between the atoms Slide 8 This picture shows the shared electrons
  • 9. Heating Silicon •We have seen that, in silicon, heat releases electrons from their bond. •This creates electron- hole pairs which are then available for conduction Slide 9
  • 10. Heating Silicon •If more heat is applies the process continues… Slide 10 •More heat… •More current… •Less resistance… •The silicon is acting as a thermistor Its resistance decreases with temperature
  • 11. Forming P-Type and N-Type material Using Silicon Doping
  • 12. Intrinsic And Extrinsic Semiconductor •Intrinsic Semiconductor: A semiconductor in its pure from is called Intrinsic Semiconductor. It is undoped. • Extrinsic Semiconductor: A semiconductor in its impure form or semi conductor which is doped is called is called extrinsic Semiconductor.
  • 13. Doping Of An Intrinsic Semiconductor • Definition: Doping is a process of adding impurity to a pure semiconductor is called the doping of a semiconductor. •When semiconductor is doped, P-Type or N-Type Semiconductor material is form. •N-Type semiconductor material have majority of electrons. •P-Type semiconductor material have majority of holes.
  • 15. N-Type Semiconductor Material Slide 15 •Phosphorus is number 15 in the periodic table •It has 15 protons and 15 electrons – 5 of these electrons are in its outer shell
  • 16. N-Type Semiconductor Material •Suppose we remove a silicon atom from the crystal lattice. •We replace it with a phosphorus atom •We now have an electron that is not bonded – it is thus free for conduction Slide 16
  • 17. N-Type Semiconductor Material •Let’s remove another silicon atom and replace it with a phosphorus atom. Slide 17 •As more electrons are available for conduction we have increased the conductivity of the material •If we now apply a potential difference across the silicon •Phosphorus is called the dopant
  • 18. Extrinsic Conduction In N-Type Semiconductor Material •A current will flow •Note: The negative electrons move towards the positive terminal Slide 18
  • 19. N-Type Silicon Material  This type of silicon is called n-type  This is because the majority charge carriers are negative electrons  A small number of minority charge carriers – holes – will exist due to electrons-hole pairs being created in the silicon atoms due to heat  The silicon is still electrically neutral as the number of protons is equal to the number of electrons Slide 19
  • 21. How P-Type Material Is Forming Using Boron Atom Slide 21 •Boron is number 5 in the periodic table •It has 5 protons and 5 electrons – 3 of these electrons are in its outer shell
  • 22. Doping – Making p-type Silicon •As before, we remove a silicon atom from the crystal lattice •This time we replace it with a boron atom •Notice we have a hole in a bond – this hole is thus free for conduction Slide 22
  • 23. Doping – Making p-type Silicon •Let’s remove another silicon atom. and replace it with another boron atom •As more holes are available for conduction we have increased the conductivity of the material Slide 23 •If we now apply a potential difference across the silicon. •Boron is the dopant in this case.
  • 24. Extrinsic Conduction – p-type silicon A current will flow – this time carried by positive holes Note: The positive holes move towards the negative terminal Slide 24
  • 25. Holes & Hole Current + + ++ + + + + + + + + + Hole Movement Electron Movement
  • 26. P-type Silicon  This type of silicon is called p-type  This is because the majority charge carriers are positive holes  A small number of minority charge carriers – electrons – will exist due to electrons-hole pairs being created in the silicon atoms due to heat  The silicon is still electrically neutral as the number of protons is equal to the number of electrons
  • 27. Donor And Acceptor Impurity Atom • Acceptor Dopant: an acceptor is a dopant atom that when added to a semiconductor can form a p-type region. •Donor Dopant: a donor is a dopant atom that, when added to a semiconductor, can form an n-type region. •Trivalent Impurity: P-type material is formed. Boron is trivalent impurity •Pentavalent Impurity: N-Type Material is formed. Phosphorus is pentavalent impurity.