SlideShare a Scribd company logo
1 of 20
Class 12 th Physics
Priyanka Jakhar
Physics Lecturer
GGIC Vijay Nagar
Ghaziabad U.P.
Semiconductor Part 1
Electronics
Electronics is the combination of two words electrons and dynamics.
Electronics is a science of flow and control of electrons in vacuum and solids.
Modern electronics is a part of solid state Physics in which flow of electrons
is channelised in solid before the introduction of modern semiconductor
electronics. Electronics was based on vacuum tubes like that diode ,triode
and tetrode valves in vacuum tubes .
The flow of electron from heating cathode was directed by various
electrodes like grid in vacuum the device based on these tubes but bulk
consume high power less reliable and have limited life also they require
vacuum for electrons flow.
First type of semiconductor diode was introduced by Sir Jagdish Chandra
Bose and Indian brain the solid state electronics was first come into light
after the invention of first practical transistor by William Shockley and his
team at Bell Labs in 1947.
Semiconductor electronics devices were started referred as they are cheap
small in size operate at low power produce almost no heat and reliable as
compared to the vacuum tube .
Energy Band In Solid :--
According to Quantum Mechanical Laws, the energies of electrons in a free atom can not have
arbitrary values but only some definite (quantized) values.
However, if an atom belongs to a crystal, then the energy levels are modified.
This modification is not appreciable in the case of energy levels of electrons in the inner
shells (completely filled).
But in the outermost shells, modification is appreciable because the electrons are shared by
many neighbouring atoms.
Due to influence of high electric field between the core of the atoms and the shared electrons,
energy levels are split-up or spread out forming energy bands.
Consider a single crystal of silicon having N atoms. Each atom can be associated with a lattice
site.
Electronic configuration of Si is 1s2, 2s2, 2p6,3s2, 3p2.(Atomic No. is 14)
When all the atoms of the Crystal are well separated ( region A ) :-- There is no interaction between
the atoms so each of an atom has same energy levels .This is represented by straight line in region A. In this
region out of four an outermost electrons 2N electrons are in 2N impossible is 3s states all have same energy
(and remaining 2N are in 6N possible 3p states ,all have same energy .Only 2N levels of 3p states are filled so
some 3p e states are empty. There is a gap between 3s and 3p states.
O
• • • • • •
• •
• •
• •
• •
2p6
2s2
1s2
3p2
3s2
Energy
a b c d Inter atomic spacing (r)
Conduction Band
Forbidden Energy Gap
Valence Band
Ion
core
state
Formation of Energy Bands in Solids:
Region A
RegionB
RegionD
RegionC
When interatomic distance reduce (region B ):-- The interaction between the atom becomes significant
the 3s and 3p States which earlier have identical energies spread out and form energy band .The gap between the
bands decrease .The different energy levels of e with continuous energy variation are called energy bands.
When interatomic distance reduce further ( region C ) :--The bands merge with each other .No energy
gap is visible since, the upper and lower energy states are mixed together .
When interatomic distance reduce further (region D ):-- The energy band again split apart . As r
becomes equal to 𝒓 𝟎 the actual interatomic distance of the Crystal the energy band of 8 N states split is apart into
two 4N field and 4N empty states separated by a gap called energy gap or energy band gap 𝑬 𝒈 .
The lower band which is completely filled by 4N valence electrons at absolute zero temperature is called Valence
band .
The upper band which is completely empty at absolute zero temperature is called conduction band .
The collection of very closely spaced energy levels is called an energy band.
Note:
1. The exact energy band picture depends on the relative orientation of atoms in a crystal.
2. If the bands in a solid are completely filled, the electrons are not permitted to move about, because there
are no vacant energy levels available.
Valence band :-- This is the lower end of a material having
valence electron .
It may be completely filled or partially empty.
The electron lying in the valence band are not usually taking part in
electrical conduction as they cannot be agitated by external electric
field.
Conduction band :-- This is the upper band of the material
with no electron at absolute zero.
It may be completely empty or partially filled .
The electrons lying in conduction band can be agitated by external
electric field .
They impart electrical conduction .
The band gap or energy gap :-- The separation between
the valence band and conduction is known as the energy gap of the
two bands.
This is the minimum energy required to move an electron from the
valence band to conduction band.
It has no electron .
It is also called the forbidden gap .
Conduction Band
Forbidden Energy Gap
Valence Band
• • • • • •
≈6 eV
Conduction Band and Valence Band in Semiconductors:--
Valence Band:--
The energy band involving the energy levels of valence electrons is known as the valence band. It is
the highest occupied energy band. When compared with insulators, the bandgap in semiconductors
is smaller. It allows the electrons in the valence band to jump into the conduction band on receiving
any external energy.
Conduction Band:--
It is the lowest unoccupied band that includes the energy levels of positive (holes) or negative (free
electrons) charge carriers. It has conducting electrons resulting in the flow of current. The
conduction band possess high energy level and are generally empty. The conduction band in
semiconductors accepts the electrons from the valence band.
The first possible energy band diagram shows that the
conduction band is only partially filled with electrons.
With a little extra energy the electrons can easily reach the
empty energy levels above the filled ones and the conduction
is possible.
The second possible energy band diagram shows that the
conduction band is overlapping with the valence band.
This is because the lowest levels in the conduction band needs
less energy than the highest levels in the valence band.
The electrons in valence band overflow into conduction band
and are free to move about in the crystal for conduction.
Conductor / Metal
Conduction Band
• • • • • •
Valence Band
Partially filled
Conduction Band
• • • • • •
Conduction Band
Valence Band
Forbidden Energy Gap
• • • •• •
Semiconductor
At absolute zero temperature, no electron has energy to jump from
valence band to conduction band and hence the crystal is an insulator.
At room temperature, some valence electrons gain energy more than the
energy gap and move to conduction band to conduct even under the
influence of a weak electric field.
As an electron leaves the valence band, it leaves some energy level in
band as unfilled.
Such unfilled regions are termed as ‘holes’ in the valence band. They
are mathematically taken as positive charge carriers.
Any movement of this region is referred to a positive hole moving from
one position to another.
Conduction Band
Valence Band
Forbidden Energy Gap ≈1 eV
Eg-Si = 1.1 eV EgGe= 0.74 eV
• • • •• •
Since 𝑬 𝒈 is small, therefore, the
fraction is sizeable for
semiconductors.
Insulators
Electrons, however heated, can not practically jump to conduction band
from valence band due to a large energy gap. Therefore, conduction
is not possible in insulators.
Eg-Diamond = 7 eV
Conduction Band
Forbidden Energy Gap
Valence Band
• • • • • •
≈6 eV
Fermi Level :-- The highest energy level which can be occupied by electrons in a crystal, at absolute 0
temperature , is called Fermi Level.
If the electrons get enough energy to go beyond this level, then conduction takes place.
Fermi energy :-- The highest possessed of free electron in a material at absolute zero known as Fermi
energy .The energy corresponding to fermi energy level is called Fermi energy.
The electron cannot interact unless possessed the Fermi level of energy.
This was named after physicist Enrico fermi, the creator of world first nuclear reactor .
At absolute zero the Fermi energy and Fermi level are equal but different at other temperatures .
The Fermi level lies between valence and conduction bands of the material .
Difference between Fermi energy and Fermi level:--
The Fermi energy is only defined at absolute zero, while the Fermi level is defined for any temperature.
The Fermi energy is an energy difference (usually corresponding to a kinetic energy), whereas the Fermi level is a
total energy level including kinetic energy and potential energy.
Fermi Level in Semiconductors:--
Fermi level (denoted by EF) is present between the valence and conduction bands.
It is the highest occupied molecular orbital at absolute zero.
The charge carriers in this state have their own quantum states and generally do not interact with
each other.
When the temperature rises above absolute zero, these charge carriers will begin to occupy states
above
Fermi level.
In a p-type semiconductor, there is an increase in the density of unfilled states. Thus,
accommodating more electrons at the lower energy levels.
BASIS OF
COMPARISON
CONDUCTOR SEMICONDUCTOR INSULATOR
Description
Conductor is a material
which permits the
electric current or heat
to pass through it.
Semi-conductor is a
material or substance
that may act as a
conductor as well as
insulators under
different conditions.
Insulators are materials
or substances which do
not allow heat or
electricity to pass
through it.
Conductivity
Have very high
conductivity, (107 Ʊ/m)
thus they can conduct
electrical current
easily.
Have intermediate
conductivity (between
10-7 Ʊ/m to 10-13 Ʊ/m),
thus they can act as
insulator and
conductor at different
conditions.
They have very low
conductivity
(1013 Ʊ/m), thus they
do not allow current
flow.
Difference Between Conductor, Insulator And Semi-Conductor
Reason For
Conductivity Or
Otherwise
The conduction in
conductors is due to
the free electrons in
metal bonding.
The conduction in
semiconductors is due
to the movement of
electrons and holes.
Non conduction is due
to absence free
electrons or holes.
Resistance Vs
Temperature
The resistance of a
conductor increases
with an increase in
temperature.
The resistance of a
semiconductor
decreases with
increase in
temperature.
Insulators have very
high resistance but it
decreases with
temperature.
Charge Carrier
In conductors,
electrons are charge
carriers.
In semiconductors,
intrinsic charge carriers
are holes and
electrons.
Insulators do not have
any charge carriers.
Valence Electrons
They have only one
valence electron in the
outermost shell.
They have four valence
electrons in the
outermost shell.
They have eight
valence electrons in
the outermost shell.
Band Gap
In conductors, there is low energy
gap between the conduction and
valence band of a conductor. It
does not need extra energy for
the conduction state.
The band gap of
semiconductor is
greater than that of
conductor but smaller
than that of an
insulator.
The band gap in
insulators is huge,
which needs an
enormous amount of
energy like lightning to
push electrons into the
conduction band.
Coefficient
Of
Resistivity
Conductors have a positive
coefficient of resistivity. Its
resistance increases with increase
in temperature.
Semiconductors have a
negative coefficient of
resistivity.
The coefficient of
resistivity of an
insulator is also
negative but it has very
huge resistance.
Absolute
Zero
Some special conductors turn
into superconductors when
supercooled down while other
have finite resistance.
The semiconductors
turn into insulators at
absolute zero.
The insulator resistance
increases when cooled
down to absolute
zero.
Valence Band &
Conduction Band
Valence band and
conduction band of
conductors is
completely filled.
Valence band is
partially empty and
conduction band is
partially filled.
Valence band of
insulators is
completely filled and
conduction band is
completely empty.
Temperature Increase
Vs Number Of Carriers
On increasing
temperature, the
number of carriers
decreases.
On increasing
temperature, the
number of carriers
increases.
On increasing
temperature, number
of carries increase.
Overlapping Of Bands
The valence and
conduction bands are
overlapped.
Valence band and
conduction band are
separated energy gap
of 1.1eV.
Both the bands get
divided by an energy
gap of 6eV -10eV.
Examples
Gold, Copper, Silver,
Aluminum etc.
Silicon, Germanium,
Selenium, Antimony,
Boron etc.
Rubber, Glass, Wood,
Mica, Plastic, Paper
etc.
Application
The metals like iron, copper,
aluminum etc that conduct
electricity are made into wires
and capable for carrying
electric current.
Semiconductors are used
every day electronic devices
such as cellphone,
computer, solar panel etc as
switches, energy converters,
amplifiers etc.
The insulators are used for
protection against high
voltages and prevention of
electrical short between
cables in circuits.
Type Of Ionic
Bonding
Conductors have metallic type
of bonding in their structure.
Semiconductors have
ionic bond and
covalent type of
bonding in their
structure.
Insulators have covalent
type of bonding in their
structure.
Effect Of Electric
Field On Current
Flow
In conductors, current flow
under the influence of electric
field takes place easily.
In semiconductors, current
flow does not take place
under the influence of
electric field.
In insulators, current flows
slowly under the influence
of electric field.
Holes and Electrons in Semiconductors:--
1. Holes and electrons are the types of charge carriers accountable
for the flow of current in semiconductors.
2. Holes (valence electrons) are the positively charged electric
charge carrier whereas electrons are the negatively charged
particles.
3. Both electrons and holes are equal in magnitude but opposite in
polarity.
Mobility of Electrons and Holes:--
1. In a semiconductor, the mobility of electrons is higher than that of the holes.
2. It is mainly because of their different band structures and scattering mechanisms.
3. Electrons travel in the conduction band whereas holes travel in the valence band.
4. When an electric field is applied, holes cannot move as freely as electrons due to
their restricted movment.
5. The elevation of electrons from their inner shells to higher shells results in the
creation of holes in semiconductors.

More Related Content

What's hot

Chapter 5 spectral lines of hydrogen atom
Chapter 5  spectral lines of hydrogen atomChapter 5  spectral lines of hydrogen atom
Chapter 5 spectral lines of hydrogen atom
Miza Kamaruzzaman
 
Electrostatics Class 12- Part 2
Electrostatics Class 12- Part 2Electrostatics Class 12- Part 2
Electrostatics Class 12- Part 2
Self-employed
 
Ray Optics Class 12 Part-2
Ray Optics Class 12 Part-2Ray Optics Class 12 Part-2
Ray Optics Class 12 Part-2
Self-employed
 
Alternating Currents Class 12
Alternating Currents Class 12Alternating Currents Class 12
Alternating Currents Class 12
Self-employed
 
Wave Optics Class 12 Part-2
Wave Optics Class 12 Part-2Wave Optics Class 12 Part-2
Wave Optics Class 12 Part-2
Self-employed
 

What's hot (20)

Dual nature of matter
Dual nature of matterDual nature of matter
Dual nature of matter
 
Chapter 5 spectral lines of hydrogen atom
Chapter 5  spectral lines of hydrogen atomChapter 5  spectral lines of hydrogen atom
Chapter 5 spectral lines of hydrogen atom
 
Class 12th Physics Photoelectric effect dual nature of matter radiations
Class 12th Physics Photoelectric effect dual nature of matter radiationsClass 12th Physics Photoelectric effect dual nature of matter radiations
Class 12th Physics Photoelectric effect dual nature of matter radiations
 
Structure of atom plus one focus area notes
Structure of atom plus one focus area notesStructure of atom plus one focus area notes
Structure of atom plus one focus area notes
 
Magnetism
MagnetismMagnetism
Magnetism
 
Electrostatics Class 12- Part 2
Electrostatics Class 12- Part 2Electrostatics Class 12- Part 2
Electrostatics Class 12- Part 2
 
CLASS XII PHYSICS Chapter 7 - wave optics
CLASS XII PHYSICS Chapter 7 - wave optics CLASS XII PHYSICS Chapter 7 - wave optics
CLASS XII PHYSICS Chapter 7 - wave optics
 
Class 12th physics magnetism ppt
Class 12th physics magnetism pptClass 12th physics magnetism ppt
Class 12th physics magnetism ppt
 
Ray Optics Class 12 Part-2
Ray Optics Class 12 Part-2Ray Optics Class 12 Part-2
Ray Optics Class 12 Part-2
 
Alternating Currents Class 12
Alternating Currents Class 12Alternating Currents Class 12
Alternating Currents Class 12
 
Oscillation 2017
Oscillation 2017Oscillation 2017
Oscillation 2017
 
Class 12th Physics wave optics ppt part 2
Class 12th Physics wave optics ppt part 2 Class 12th Physics wave optics ppt part 2
Class 12th Physics wave optics ppt part 2
 
Hydrogen atom
Hydrogen atomHydrogen atom
Hydrogen atom
 
Dual nature of radiation & matter
Dual nature of radiation & matterDual nature of radiation & matter
Dual nature of radiation & matter
 
ELECTROSTATIC POTENTIAL ENERGY
ELECTROSTATIC  POTENTIAL ENERGYELECTROSTATIC  POTENTIAL ENERGY
ELECTROSTATIC POTENTIAL ENERGY
 
Class 12th Physics Atom nuclei PPt
Class 12th Physics Atom nuclei PPtClass 12th Physics Atom nuclei PPt
Class 12th Physics Atom nuclei PPt
 
Electrostatics
ElectrostaticsElectrostatics
Electrostatics
 
Wave functions
Wave functionsWave functions
Wave functions
 
Wave Optics Class 12 Part-2
Wave Optics Class 12 Part-2Wave Optics Class 12 Part-2
Wave Optics Class 12 Part-2
 
PHY PUC 2 MOVING CHARGE AND MAGNETISM
PHY PUC 2 MOVING CHARGE AND MAGNETISMPHY PUC 2 MOVING CHARGE AND MAGNETISM
PHY PUC 2 MOVING CHARGE AND MAGNETISM
 

Similar to Class 12 th semiconductor part 1

semiconductors_jee_eng. .pdf
semiconductors_jee_eng.               .pdfsemiconductors_jee_eng.               .pdf
semiconductors_jee_eng. .pdf
RITASINGH445812
 
B.tech sem i engineering physics u ii chapter 1-band theory of solid
B.tech sem i engineering physics u ii chapter 1-band theory of solidB.tech sem i engineering physics u ii chapter 1-band theory of solid
B.tech sem i engineering physics u ii chapter 1-band theory of solid
Rai University
 
Diploma sem 2 applied science physics-unit 3-chap-1 band theory of solid
Diploma sem 2 applied science physics-unit 3-chap-1 band theory of solidDiploma sem 2 applied science physics-unit 3-chap-1 band theory of solid
Diploma sem 2 applied science physics-unit 3-chap-1 band theory of solid
Rai University
 
B.Tech sem I Engineering Physics U-II Chapter 1-Band theory of solid
B.Tech sem I Engineering Physics U-II Chapter 1-Band theory of solidB.Tech sem I Engineering Physics U-II Chapter 1-Band theory of solid
B.Tech sem I Engineering Physics U-II Chapter 1-Band theory of solid
Abhi Hirpara
 
358011521-PPT-ELECTRICAL-PROPERTIES-band theory.pptx
358011521-PPT-ELECTRICAL-PROPERTIES-band theory.pptx358011521-PPT-ELECTRICAL-PROPERTIES-band theory.pptx
358011521-PPT-ELECTRICAL-PROPERTIES-band theory.pptx
khoi0209
 
Electronic device lecture1
Electronic device lecture1Electronic device lecture1
Electronic device lecture1
Neeraj Gupta
 

Similar to Class 12 th semiconductor part 1 (20)

Solids_And_Semiconductor_Devices_1.ppt
Solids_And_Semiconductor_Devices_1.pptSolids_And_Semiconductor_Devices_1.ppt
Solids_And_Semiconductor_Devices_1.ppt
 
Class 12th Solids and semiconductor devices part 1
Class 12th Solids and semiconductor devices part 1Class 12th Solids and semiconductor devices part 1
Class 12th Solids and semiconductor devices part 1
 
Solids & Semiconductor Devices
Solids & Semiconductor DevicesSolids & Semiconductor Devices
Solids & Semiconductor Devices
 
Solids_And_Semiconductor_Devices_123.pdf
Solids_And_Semiconductor_Devices_123.pdfSolids_And_Semiconductor_Devices_123.pdf
Solids_And_Semiconductor_Devices_123.pdf
 
semiconductors_jee_eng. .pdf
semiconductors_jee_eng.               .pdfsemiconductors_jee_eng.               .pdf
semiconductors_jee_eng. .pdf
 
solids_and_semiconductor_devices_1.ppt
solids_and_semiconductor_devices_1.pptsolids_and_semiconductor_devices_1.ppt
solids_and_semiconductor_devices_1.ppt
 
B.tech sem i engineering physics u ii chapter 1-band theory of solid
B.tech sem i engineering physics u ii chapter 1-band theory of solidB.tech sem i engineering physics u ii chapter 1-band theory of solid
B.tech sem i engineering physics u ii chapter 1-band theory of solid
 
Diploma sem 2 applied science physics-unit 3-chap-1 band theory of solid
Diploma sem 2 applied science physics-unit 3-chap-1 band theory of solidDiploma sem 2 applied science physics-unit 3-chap-1 band theory of solid
Diploma sem 2 applied science physics-unit 3-chap-1 band theory of solid
 
Semiconductors
SemiconductorsSemiconductors
Semiconductors
 
Semiconcuctor devices introduction
Semiconcuctor devices  introductionSemiconcuctor devices  introduction
Semiconcuctor devices introduction
 
B.Tech sem I Engineering Physics U-II Chapter 1-Band theory of solid
B.Tech sem I Engineering Physics U-II Chapter 1-Band theory of solidB.Tech sem I Engineering Physics U-II Chapter 1-Band theory of solid
B.Tech sem I Engineering Physics U-II Chapter 1-Band theory of solid
 
Module 1 Semiconductors (1).pptx
Module 1  Semiconductors (1).pptxModule 1  Semiconductors (1).pptx
Module 1 Semiconductors (1).pptx
 
Semiconductors
SemiconductorsSemiconductors
Semiconductors
 
358011521-PPT-ELECTRICAL-PROPERTIES-band theory.pptx
358011521-PPT-ELECTRICAL-PROPERTIES-band theory.pptx358011521-PPT-ELECTRICAL-PROPERTIES-band theory.pptx
358011521-PPT-ELECTRICAL-PROPERTIES-band theory.pptx
 
semiconductor and hall effect.pptx chemistry .....
semiconductor and hall effect.pptx chemistry .....semiconductor and hall effect.pptx chemistry .....
semiconductor and hall effect.pptx chemistry .....
 
9m electronic devices
9m electronic devices9m electronic devices
9m electronic devices
 
Bandtheory of solids
Bandtheory of solidsBandtheory of solids
Bandtheory of solids
 
Basic electronics
Basic electronicsBasic electronics
Basic electronics
 
Electronic device lecture1
Electronic device lecture1Electronic device lecture1
Electronic device lecture1
 
Electronic device lecture1
Electronic device lecture1Electronic device lecture1
Electronic device lecture1
 

More from Priyanka Jakhar

More from Priyanka Jakhar (20)

PHYSICAL WORLD part 2
PHYSICAL WORLD part 2PHYSICAL WORLD part 2
PHYSICAL WORLD part 2
 
Capacitor
Capacitor Capacitor
Capacitor
 
Physical world part 1
Physical world part 1Physical world part 1
Physical world part 1
 
PHYSICAL WORLD part 1
PHYSICAL WORLD part 1PHYSICAL WORLD part 1
PHYSICAL WORLD part 1
 
Mutual induction
Mutual induction    Mutual induction
Mutual induction
 
Eddy current
Eddy currentEddy current
Eddy current
 
Ultasonic sensor
Ultasonic sensorUltasonic sensor
Ultasonic sensor
 
electromagnetic induction ( part 2 )
electromagnetic induction ( part 2 )electromagnetic induction ( part 2 )
electromagnetic induction ( part 2 )
 
electromagnetic induction ( part 1 )
electromagnetic induction ( part 1 )electromagnetic induction ( part 1 )
electromagnetic induction ( part 1 )
 
Breadboard
BreadboardBreadboard
Breadboard
 
Jumper wires
Jumper wiresJumper wires
Jumper wires
 
Earths magnetism part 1
Earths magnetism part 1Earths magnetism part 1
Earths magnetism part 1
 
Earths magnetism
Earths magnetismEarths magnetism
Earths magnetism
 
Superconductor
SuperconductorSuperconductor
Superconductor
 
VandE GRAFF generator
VandE GRAFF generatorVandE GRAFF generator
VandE GRAFF generator
 
Electromagnetic Wave
Electromagnetic Wave Electromagnetic Wave
Electromagnetic Wave
 
Transformer
TransformerTransformer
Transformer
 
Alternating Current
Alternating CurrentAlternating Current
Alternating Current
 
Ac generator
Ac generatorAc generator
Ac generator
 
Class 12 th semiconductor part 4
Class 12 th semiconductor part 4Class 12 th semiconductor part 4
Class 12 th semiconductor part 4
 

Recently uploaded

Spellings Wk 4 and Wk 5 for Grade 4 at CAPS
Spellings Wk 4 and Wk 5 for Grade 4 at CAPSSpellings Wk 4 and Wk 5 for Grade 4 at CAPS
Spellings Wk 4 and Wk 5 for Grade 4 at CAPS
AnaAcapella
 

Recently uploaded (20)

Beyond_Borders_Understanding_Anime_and_Manga_Fandom_A_Comprehensive_Audience_...
Beyond_Borders_Understanding_Anime_and_Manga_Fandom_A_Comprehensive_Audience_...Beyond_Borders_Understanding_Anime_and_Manga_Fandom_A_Comprehensive_Audience_...
Beyond_Borders_Understanding_Anime_and_Manga_Fandom_A_Comprehensive_Audience_...
 
dusjagr & nano talk on open tools for agriculture research and learning
dusjagr & nano talk on open tools for agriculture research and learningdusjagr & nano talk on open tools for agriculture research and learning
dusjagr & nano talk on open tools for agriculture research and learning
 
Accessible Digital Futures project (20/03/2024)
Accessible Digital Futures project (20/03/2024)Accessible Digital Futures project (20/03/2024)
Accessible Digital Futures project (20/03/2024)
 
PANDITA RAMABAI- Indian political thought GENDER.pptx
PANDITA RAMABAI- Indian political thought GENDER.pptxPANDITA RAMABAI- Indian political thought GENDER.pptx
PANDITA RAMABAI- Indian political thought GENDER.pptx
 
UGC NET Paper 1 Unit 7 DATA INTERPRETATION.pdf
UGC NET Paper 1 Unit 7 DATA INTERPRETATION.pdfUGC NET Paper 1 Unit 7 DATA INTERPRETATION.pdf
UGC NET Paper 1 Unit 7 DATA INTERPRETATION.pdf
 
Play hard learn harder: The Serious Business of Play
Play hard learn harder:  The Serious Business of PlayPlay hard learn harder:  The Serious Business of Play
Play hard learn harder: The Serious Business of Play
 
What is 3 Way Matching Process in Odoo 17.pptx
What is 3 Way Matching Process in Odoo 17.pptxWhat is 3 Way Matching Process in Odoo 17.pptx
What is 3 Way Matching Process in Odoo 17.pptx
 
OS-operating systems- ch05 (CPU Scheduling) ...
OS-operating systems- ch05 (CPU Scheduling) ...OS-operating systems- ch05 (CPU Scheduling) ...
OS-operating systems- ch05 (CPU Scheduling) ...
 
Unit 3 Emotional Intelligence and Spiritual Intelligence.pdf
Unit 3 Emotional Intelligence and Spiritual Intelligence.pdfUnit 3 Emotional Intelligence and Spiritual Intelligence.pdf
Unit 3 Emotional Intelligence and Spiritual Intelligence.pdf
 
FSB Advising Checklist - Orientation 2024
FSB Advising Checklist - Orientation 2024FSB Advising Checklist - Orientation 2024
FSB Advising Checklist - Orientation 2024
 
Spellings Wk 4 and Wk 5 for Grade 4 at CAPS
Spellings Wk 4 and Wk 5 for Grade 4 at CAPSSpellings Wk 4 and Wk 5 for Grade 4 at CAPS
Spellings Wk 4 and Wk 5 for Grade 4 at CAPS
 
How to Create and Manage Wizard in Odoo 17
How to Create and Manage Wizard in Odoo 17How to Create and Manage Wizard in Odoo 17
How to Create and Manage Wizard in Odoo 17
 
80 ĐỀ THI THỬ TUYỂN SINH TIẾNG ANH VÀO 10 SỞ GD – ĐT THÀNH PHỐ HỒ CHÍ MINH NĂ...
80 ĐỀ THI THỬ TUYỂN SINH TIẾNG ANH VÀO 10 SỞ GD – ĐT THÀNH PHỐ HỒ CHÍ MINH NĂ...80 ĐỀ THI THỬ TUYỂN SINH TIẾNG ANH VÀO 10 SỞ GD – ĐT THÀNH PHỐ HỒ CHÍ MINH NĂ...
80 ĐỀ THI THỬ TUYỂN SINH TIẾNG ANH VÀO 10 SỞ GD – ĐT THÀNH PHỐ HỒ CHÍ MINH NĂ...
 
Graduate Outcomes Presentation Slides - English
Graduate Outcomes Presentation Slides - EnglishGraduate Outcomes Presentation Slides - English
Graduate Outcomes Presentation Slides - English
 
Jamworks pilot and AI at Jisc (20/03/2024)
Jamworks pilot and AI at Jisc (20/03/2024)Jamworks pilot and AI at Jisc (20/03/2024)
Jamworks pilot and AI at Jisc (20/03/2024)
 
TỔNG ÔN TẬP THI VÀO LỚP 10 MÔN TIẾNG ANH NĂM HỌC 2023 - 2024 CÓ ĐÁP ÁN (NGỮ Â...
TỔNG ÔN TẬP THI VÀO LỚP 10 MÔN TIẾNG ANH NĂM HỌC 2023 - 2024 CÓ ĐÁP ÁN (NGỮ Â...TỔNG ÔN TẬP THI VÀO LỚP 10 MÔN TIẾNG ANH NĂM HỌC 2023 - 2024 CÓ ĐÁP ÁN (NGỮ Â...
TỔNG ÔN TẬP THI VÀO LỚP 10 MÔN TIẾNG ANH NĂM HỌC 2023 - 2024 CÓ ĐÁP ÁN (NGỮ Â...
 
Understanding Accommodations and Modifications
Understanding  Accommodations and ModificationsUnderstanding  Accommodations and Modifications
Understanding Accommodations and Modifications
 
REMIFENTANIL: An Ultra short acting opioid.pptx
REMIFENTANIL: An Ultra short acting opioid.pptxREMIFENTANIL: An Ultra short acting opioid.pptx
REMIFENTANIL: An Ultra short acting opioid.pptx
 
Our Environment Class 10 Science Notes pdf
Our Environment Class 10 Science Notes pdfOur Environment Class 10 Science Notes pdf
Our Environment Class 10 Science Notes pdf
 
COMMUNICATING NEGATIVE NEWS - APPROACHES .pptx
COMMUNICATING NEGATIVE NEWS - APPROACHES .pptxCOMMUNICATING NEGATIVE NEWS - APPROACHES .pptx
COMMUNICATING NEGATIVE NEWS - APPROACHES .pptx
 

Class 12 th semiconductor part 1

  • 1. Class 12 th Physics Priyanka Jakhar Physics Lecturer GGIC Vijay Nagar Ghaziabad U.P. Semiconductor Part 1
  • 2. Electronics Electronics is the combination of two words electrons and dynamics. Electronics is a science of flow and control of electrons in vacuum and solids. Modern electronics is a part of solid state Physics in which flow of electrons is channelised in solid before the introduction of modern semiconductor electronics. Electronics was based on vacuum tubes like that diode ,triode and tetrode valves in vacuum tubes . The flow of electron from heating cathode was directed by various electrodes like grid in vacuum the device based on these tubes but bulk consume high power less reliable and have limited life also they require vacuum for electrons flow. First type of semiconductor diode was introduced by Sir Jagdish Chandra Bose and Indian brain the solid state electronics was first come into light after the invention of first practical transistor by William Shockley and his team at Bell Labs in 1947. Semiconductor electronics devices were started referred as they are cheap small in size operate at low power produce almost no heat and reliable as compared to the vacuum tube .
  • 3.
  • 4. Energy Band In Solid :-- According to Quantum Mechanical Laws, the energies of electrons in a free atom can not have arbitrary values but only some definite (quantized) values. However, if an atom belongs to a crystal, then the energy levels are modified. This modification is not appreciable in the case of energy levels of electrons in the inner shells (completely filled). But in the outermost shells, modification is appreciable because the electrons are shared by many neighbouring atoms. Due to influence of high electric field between the core of the atoms and the shared electrons, energy levels are split-up or spread out forming energy bands. Consider a single crystal of silicon having N atoms. Each atom can be associated with a lattice site. Electronic configuration of Si is 1s2, 2s2, 2p6,3s2, 3p2.(Atomic No. is 14) When all the atoms of the Crystal are well separated ( region A ) :-- There is no interaction between the atoms so each of an atom has same energy levels .This is represented by straight line in region A. In this region out of four an outermost electrons 2N electrons are in 2N impossible is 3s states all have same energy (and remaining 2N are in 6N possible 3p states ,all have same energy .Only 2N levels of 3p states are filled so some 3p e states are empty. There is a gap between 3s and 3p states.
  • 5. O • • • • • • • • • • • • • • 2p6 2s2 1s2 3p2 3s2 Energy a b c d Inter atomic spacing (r) Conduction Band Forbidden Energy Gap Valence Band Ion core state Formation of Energy Bands in Solids: Region A RegionB RegionD RegionC
  • 6. When interatomic distance reduce (region B ):-- The interaction between the atom becomes significant the 3s and 3p States which earlier have identical energies spread out and form energy band .The gap between the bands decrease .The different energy levels of e with continuous energy variation are called energy bands. When interatomic distance reduce further ( region C ) :--The bands merge with each other .No energy gap is visible since, the upper and lower energy states are mixed together . When interatomic distance reduce further (region D ):-- The energy band again split apart . As r becomes equal to 𝒓 𝟎 the actual interatomic distance of the Crystal the energy band of 8 N states split is apart into two 4N field and 4N empty states separated by a gap called energy gap or energy band gap 𝑬 𝒈 . The lower band which is completely filled by 4N valence electrons at absolute zero temperature is called Valence band . The upper band which is completely empty at absolute zero temperature is called conduction band . The collection of very closely spaced energy levels is called an energy band. Note: 1. The exact energy band picture depends on the relative orientation of atoms in a crystal. 2. If the bands in a solid are completely filled, the electrons are not permitted to move about, because there are no vacant energy levels available.
  • 7.
  • 8. Valence band :-- This is the lower end of a material having valence electron . It may be completely filled or partially empty. The electron lying in the valence band are not usually taking part in electrical conduction as they cannot be agitated by external electric field. Conduction band :-- This is the upper band of the material with no electron at absolute zero. It may be completely empty or partially filled . The electrons lying in conduction band can be agitated by external electric field . They impart electrical conduction . The band gap or energy gap :-- The separation between the valence band and conduction is known as the energy gap of the two bands. This is the minimum energy required to move an electron from the valence band to conduction band. It has no electron . It is also called the forbidden gap . Conduction Band Forbidden Energy Gap Valence Band • • • • • • ≈6 eV
  • 9. Conduction Band and Valence Band in Semiconductors:-- Valence Band:-- The energy band involving the energy levels of valence electrons is known as the valence band. It is the highest occupied energy band. When compared with insulators, the bandgap in semiconductors is smaller. It allows the electrons in the valence band to jump into the conduction band on receiving any external energy. Conduction Band:-- It is the lowest unoccupied band that includes the energy levels of positive (holes) or negative (free electrons) charge carriers. It has conducting electrons resulting in the flow of current. The conduction band possess high energy level and are generally empty. The conduction band in semiconductors accepts the electrons from the valence band.
  • 10. The first possible energy band diagram shows that the conduction band is only partially filled with electrons. With a little extra energy the electrons can easily reach the empty energy levels above the filled ones and the conduction is possible. The second possible energy band diagram shows that the conduction band is overlapping with the valence band. This is because the lowest levels in the conduction band needs less energy than the highest levels in the valence band. The electrons in valence band overflow into conduction band and are free to move about in the crystal for conduction. Conductor / Metal Conduction Band • • • • • • Valence Band Partially filled Conduction Band • • • • • • Conduction Band Valence Band Forbidden Energy Gap • • • •• •
  • 11. Semiconductor At absolute zero temperature, no electron has energy to jump from valence band to conduction band and hence the crystal is an insulator. At room temperature, some valence electrons gain energy more than the energy gap and move to conduction band to conduct even under the influence of a weak electric field. As an electron leaves the valence band, it leaves some energy level in band as unfilled. Such unfilled regions are termed as ‘holes’ in the valence band. They are mathematically taken as positive charge carriers. Any movement of this region is referred to a positive hole moving from one position to another. Conduction Band Valence Band Forbidden Energy Gap ≈1 eV Eg-Si = 1.1 eV EgGe= 0.74 eV • • • •• • Since 𝑬 𝒈 is small, therefore, the fraction is sizeable for semiconductors. Insulators Electrons, however heated, can not practically jump to conduction band from valence band due to a large energy gap. Therefore, conduction is not possible in insulators. Eg-Diamond = 7 eV Conduction Band Forbidden Energy Gap Valence Band • • • • • • ≈6 eV
  • 12. Fermi Level :-- The highest energy level which can be occupied by electrons in a crystal, at absolute 0 temperature , is called Fermi Level. If the electrons get enough energy to go beyond this level, then conduction takes place. Fermi energy :-- The highest possessed of free electron in a material at absolute zero known as Fermi energy .The energy corresponding to fermi energy level is called Fermi energy. The electron cannot interact unless possessed the Fermi level of energy. This was named after physicist Enrico fermi, the creator of world first nuclear reactor . At absolute zero the Fermi energy and Fermi level are equal but different at other temperatures . The Fermi level lies between valence and conduction bands of the material .
  • 13. Difference between Fermi energy and Fermi level:-- The Fermi energy is only defined at absolute zero, while the Fermi level is defined for any temperature. The Fermi energy is an energy difference (usually corresponding to a kinetic energy), whereas the Fermi level is a total energy level including kinetic energy and potential energy. Fermi Level in Semiconductors:-- Fermi level (denoted by EF) is present between the valence and conduction bands. It is the highest occupied molecular orbital at absolute zero. The charge carriers in this state have their own quantum states and generally do not interact with each other. When the temperature rises above absolute zero, these charge carriers will begin to occupy states above Fermi level. In a p-type semiconductor, there is an increase in the density of unfilled states. Thus, accommodating more electrons at the lower energy levels.
  • 14. BASIS OF COMPARISON CONDUCTOR SEMICONDUCTOR INSULATOR Description Conductor is a material which permits the electric current or heat to pass through it. Semi-conductor is a material or substance that may act as a conductor as well as insulators under different conditions. Insulators are materials or substances which do not allow heat or electricity to pass through it. Conductivity Have very high conductivity, (107 Ʊ/m) thus they can conduct electrical current easily. Have intermediate conductivity (between 10-7 Ʊ/m to 10-13 Ʊ/m), thus they can act as insulator and conductor at different conditions. They have very low conductivity (1013 Ʊ/m), thus they do not allow current flow. Difference Between Conductor, Insulator And Semi-Conductor
  • 15. Reason For Conductivity Or Otherwise The conduction in conductors is due to the free electrons in metal bonding. The conduction in semiconductors is due to the movement of electrons and holes. Non conduction is due to absence free electrons or holes. Resistance Vs Temperature The resistance of a conductor increases with an increase in temperature. The resistance of a semiconductor decreases with increase in temperature. Insulators have very high resistance but it decreases with temperature. Charge Carrier In conductors, electrons are charge carriers. In semiconductors, intrinsic charge carriers are holes and electrons. Insulators do not have any charge carriers. Valence Electrons They have only one valence electron in the outermost shell. They have four valence electrons in the outermost shell. They have eight valence electrons in the outermost shell.
  • 16. Band Gap In conductors, there is low energy gap between the conduction and valence band of a conductor. It does not need extra energy for the conduction state. The band gap of semiconductor is greater than that of conductor but smaller than that of an insulator. The band gap in insulators is huge, which needs an enormous amount of energy like lightning to push electrons into the conduction band. Coefficient Of Resistivity Conductors have a positive coefficient of resistivity. Its resistance increases with increase in temperature. Semiconductors have a negative coefficient of resistivity. The coefficient of resistivity of an insulator is also negative but it has very huge resistance. Absolute Zero Some special conductors turn into superconductors when supercooled down while other have finite resistance. The semiconductors turn into insulators at absolute zero. The insulator resistance increases when cooled down to absolute zero.
  • 17. Valence Band & Conduction Band Valence band and conduction band of conductors is completely filled. Valence band is partially empty and conduction band is partially filled. Valence band of insulators is completely filled and conduction band is completely empty. Temperature Increase Vs Number Of Carriers On increasing temperature, the number of carriers decreases. On increasing temperature, the number of carriers increases. On increasing temperature, number of carries increase. Overlapping Of Bands The valence and conduction bands are overlapped. Valence band and conduction band are separated energy gap of 1.1eV. Both the bands get divided by an energy gap of 6eV -10eV. Examples Gold, Copper, Silver, Aluminum etc. Silicon, Germanium, Selenium, Antimony, Boron etc. Rubber, Glass, Wood, Mica, Plastic, Paper etc.
  • 18. Application The metals like iron, copper, aluminum etc that conduct electricity are made into wires and capable for carrying electric current. Semiconductors are used every day electronic devices such as cellphone, computer, solar panel etc as switches, energy converters, amplifiers etc. The insulators are used for protection against high voltages and prevention of electrical short between cables in circuits. Type Of Ionic Bonding Conductors have metallic type of bonding in their structure. Semiconductors have ionic bond and covalent type of bonding in their structure. Insulators have covalent type of bonding in their structure. Effect Of Electric Field On Current Flow In conductors, current flow under the influence of electric field takes place easily. In semiconductors, current flow does not take place under the influence of electric field. In insulators, current flows slowly under the influence of electric field.
  • 19.
  • 20. Holes and Electrons in Semiconductors:-- 1. Holes and electrons are the types of charge carriers accountable for the flow of current in semiconductors. 2. Holes (valence electrons) are the positively charged electric charge carrier whereas electrons are the negatively charged particles. 3. Both electrons and holes are equal in magnitude but opposite in polarity. Mobility of Electrons and Holes:-- 1. In a semiconductor, the mobility of electrons is higher than that of the holes. 2. It is mainly because of their different band structures and scattering mechanisms. 3. Electrons travel in the conduction band whereas holes travel in the valence band. 4. When an electric field is applied, holes cannot move as freely as electrons due to their restricted movment. 5. The elevation of electrons from their inner shells to higher shells results in the creation of holes in semiconductors.