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Optical Emission
From Semiconductor



                  Md
     Presented
                 Manzar
        By
                 Nezami
Point Of Discussion
Explain with the help of energy band
 structure, the process of optical emission from
 semiconductor.
To allow consideration of semiconductor optical
 sources it is necessary to review some of the
 properties of semiconductor
 materials, especially with regard to p-n junction.
semiconductor



Intrinsic       Extrinsic
Intrinsic Semiconductor: A perfect
 semiconductor crystal containing no impurities
 and lattice effect.
Extrinsic Semiconductor: A semiconductor
 crystal which is made up by the process of
 doping, i.e. adding impurity to it.
For a semiconductor in thermal equilibrium the
 energy level occupation is described by fermi
 dirac distribution function.
 Consequently the probability p(E) that an
 electron gains sufficient thermal energy at an
 absolute temperature T such that it will be found
 occupying a particular energy level E, is given by
 the fermi-dirac distribution.
           P(E)=1/{1+exp(E-Ef )/kT}
• To create an extrinsic semicondutor the material
  is doped with impurity atoms which creates
  either more free electrons (donor impurity) or
  holes(acceptor impurity)
The p-n junction diode
The p-n junction diode is formed by creating
 adjoining p and n type semiconductor layers in
 single crystal.
A thin depletion region is formed at the junction
 through carrier recombination.
This establishes a potential barrier between the p
 and n type regions which restricts the inter diffusion
 of majority carriers from their respective regions.
An external applied voltage form current flow
 through the device as they continuously diffuse away
 from the interface.
However, this situation in suitable semiconductor
 allows carrier recombination with the emission of
 light.
Opto ppt
Opto ppt

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Opto ppt

  • 1. Optical Emission From Semiconductor Md Presented Manzar By Nezami
  • 2. Point Of Discussion Explain with the help of energy band structure, the process of optical emission from semiconductor.
  • 3. To allow consideration of semiconductor optical sources it is necessary to review some of the properties of semiconductor materials, especially with regard to p-n junction.
  • 5. Intrinsic Semiconductor: A perfect semiconductor crystal containing no impurities and lattice effect. Extrinsic Semiconductor: A semiconductor crystal which is made up by the process of doping, i.e. adding impurity to it.
  • 6.
  • 7. For a semiconductor in thermal equilibrium the energy level occupation is described by fermi dirac distribution function.  Consequently the probability p(E) that an electron gains sufficient thermal energy at an absolute temperature T such that it will be found occupying a particular energy level E, is given by the fermi-dirac distribution.  P(E)=1/{1+exp(E-Ef )/kT}
  • 8.
  • 9. • To create an extrinsic semicondutor the material is doped with impurity atoms which creates either more free electrons (donor impurity) or holes(acceptor impurity)
  • 10.
  • 11. The p-n junction diode The p-n junction diode is formed by creating adjoining p and n type semiconductor layers in single crystal. A thin depletion region is formed at the junction through carrier recombination. This establishes a potential barrier between the p and n type regions which restricts the inter diffusion of majority carriers from their respective regions. An external applied voltage form current flow through the device as they continuously diffuse away from the interface. However, this situation in suitable semiconductor allows carrier recombination with the emission of light.