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Friday, March 1, 2013

Semiconductor and Electronic Devices Theory | Notes

Energy band diagrams
  • In metals, the conduction band and valence band partly overlap each other and there is no forbidden energy gap or there is partially filled conduction band.
Energy band diagram of metals
Energy band diagram of metals
  • In insulators, the conduction band is empty and valence band is completely filled and forbidden gap is quite large ~ 6 eV. No electron from valence band can cross over to conduction band at room temperature, even if electric field is applied. Hence there is no conductivity of the insulators.
Energy band diagram of insulators
Energy band diagram of insulators
  • In semiconductors, the conduction band is empty and valence band is totally filled. But the forbidden gap between conduction band and valence band is quite small, which is about 1 eV. No electron from valence band can cross over to conduction band. Therefore, the semiconductor behaves as insulator. At room temperature, some electrons in the valence band acquire thermal energy, greater than energy gap of 1 eV and jump over to the conduction band where they are free to move under the influence of even a small electric field. Due to which, the semiconductor acquires small conductivity at room temperature
Energy band diagram of semiconductors
Energy band diagram of semiconductors
            
                    
Differences

Distinction between Intrinsic and Extrinsic Semiconductor
Intrinsic
Extrinsic
1
It is pure semiconducting material and no impurity atoms are added to it
1
It is prepared by doping a small quantity of impurity atoms to the pure semiconducting material.
2
Examples are crystalline forms of pure silicon and germanium.
2
Examples are silicon and germanium crystals with impurity atoms of  arsenic, antimony, phosphorous etc. or indium, boron, aluminum etc.
3
The number of free electron in conduction band and the number of holes in valence band is exactly equal and very small indeed.
3
The number of free electrons and holes is never equal. There is excess of electrons in n-type semiconductors and excess of holes in p-type semiconductors.
4
Its electrical conductivity is low
4
Its electrical conductivity is high.
5
Its electrical conductivity is a function of temperature alone.
5
Its electrical conductivity depends upon the temperature as well as on the quantity of impurity atoms doped in the structure.



Distinction between n-type and p-type semiconductors
n-type semiconductors
p-type semiconductors
1
It is an extrinsic semiconductors which is obtained by doping the impurity atoms of Vth group of periodic table to the pure germanium or silicon semiconductor.
1
It is an intrinsic semiconductors which is obtained by doping the impurity atoms of III group of periodic table to the pure germanium or silicon semiconductor.
2
The impurity atoms added, provide extra electrons in the structure, and are called donor atoms.
2
The impurity atoms added, create vacancies of electrons (i.e. holes) in the structure and are called acceptor atoms.
3
The electrons are majority carriers and holes are minority carriers.
3
The holes are majority carriers and electrons are minority carriers.
4
The electron density (ne) is much greater than the hole density (nh)i.e. ne>>(nh)
4
The hole density (ne) is much greater than the electron density (nh)i.e. nh>> ne
5
The donor energy level is close to the conduction band and far away from valence band.
5
The acceptor energy level is close to valence band and is far away from the conduction band.
6
The Fermi energy level lies in between the donor energy level and conduction band.
6
The Fermi energy level lies in between the acceptor energy level and valence band.

P-n junction diode

  • Two important processes occur during the formation of p-n junction, diffusion and drift.
  • The motion of majority charge carriers give rise to diffusion current.
  • Due to the positive space charge on n-side junction and negative space charge region on p-side the electric field is set up and potential barrier develops at the junction Due to electric field electrons on p-side moves to n and holes from n-side to p-side which is called drift current.
  • In equilibrium state, there is no current across p-n junction and potential barrier across p-n junction has maximum value .
  • The width of the depletion region and magnitude of barrier potential depends on the nature of semiconductor and doping concentration on two sides of p-n junction –

Forward Bias
  • P-n junction is forward biased when p-type is connected to the positive terminal of battery and n-type connected to negative terminal of battery.
  • Potential barrier height is reduced and width of depletion layer decreases.
  • Resistance of p-n junction is low to the flow of current in this condition.

Reverse Bias

  • P-n junction is reverse biased when p-type connected  to the negative terminal of battery and n-type connected to positive terminal of battery.
  • Resistance of p-n junction is high to the flow of current in this condition.
  • Potential barrier height is increased and width of depletion layer increases


Diode Characteristics:
 Diode Characteristics circuit diagram under forward bias
 Diode Characteristics circuit diagram under forward bias
 Diode Characteristics circuit diagram under reverse bias
 Diode Characteristics circuit diagram under reverse bias

Diode Characteristics graph under reverse bias
Diode Characteristics graph under reverse bias      
       
Diode Characteristics graph under forward bias
Diode Characteristics graph under forward bias
















Rectification

p-n junction diode as half wave rectifier
p-n junction diode as half wave rectifier
p-n junction diode as full wave rectifier
p-n junction diode as full wave rectifier


Zener diode as a voltage regulator
Zener diode as a voltage regulator



Photonic(Optoelectronic) Devices

                           LED
PHOTODIODE
SOLARCELL
Symbol of LED
Symbol of LED
Forward biased
Symbol of Photodiode
Symbol of Photodiode
Reverse biased
Symbol of Solar Cell
Symbol of Solar Cell
No external baising,It generates emf when solar radiation falls on it.
Recombination of electrons and holes  take place at the junction and emits electromagnetic radiations
Energy is supplied by light to take an electron from valence band to conduction band.
Generation of emf by solar cells is due to three basic process generation of electron-hole pair,separation and collection
It is used in Burglar alarm, remote control

LED Characteristics graph
LED Characteristics graph
It is used in photo detectors in communication
Photodiode Characteristics graph
Photodiode Characteristics graph

It is used in satellites,space vechicles calculators.
Solar Cell Characteristics graph
Solar Cell Characteristics graph





Transistor

npn transistor and pnp transistor
npn transistor and pnp transistor
     There are two types of transistor – NPN & PNP
     Applications of transistor
  1.     Transistor as a switch  
  2.     Transistor as an amplifier    
  3.     Transistor as an oscillator





Transistor- Switch
   When a transistor is used in cut off or saturated state, it behaves as a switch.
Transistor as switch, Cutoff region, Active Region, Saturation Region
Transistor as switch, Cutoff region, Active Region, Saturation Region



Transistor as an Amplifier

Current gain, Voltage gain and Power gain
Current gain, Voltage gain and Power gain
An amplifier is a device which is used for increasing the amplitude of variation of alternating voltage or current or power,thus it produces an enlarged version of the input signal. 

For Circuit diagram refer Ncert diagram




Transistor-Oscillator-
      In an oscillator, we get ac output without any external input signal. In other words, the output in an oscillator is self- sustained. Oscillator converts D.C into A.C

Digital Electronics –Logic Gates
      The three basic Logic Gates are

(1)  OR Gate 
OR gate AND gate NOT gate
OR gate, AND gate & NOT gate
                            OUTPUT Y= A + B 
 (2) AND Gate
                             OUTPUT Y=A.B
 (3) NOT GATE
                             OUTPUT  Y=Y’



COMBINATION OF GATES
                                                        __
 (1)   NOR GATE--OUT PUT Y = A+B              
                                                        __
(2)   NAND GATE--OUT PUT Y= A .B




             









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