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Avalanche Photodiode APD

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... kinetic energy (greater than Eg) to impact-ionize some of the Si covalent bonds ... be accelerated by high fields to high kinetic energies to cause further impact ... – PowerPoint PPT presentation

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Title: Avalanche Photodiode APD


1
Avalanche Photodiode (APD)
  • Attributes high speed and internal gain
  • Good for communications
  • A thin side layer is exposed through a
    window to achieve illumination.
  • 3 p type layers follow this and terminate at the
    electrode.
  • These p-type layers have different doping levels
    in order to modify the field distribution across
    the diode.
  • 1st p-type region is a thin layer
  • 2nd p-type region is a thick, lightly dope
    layer. (almost intrinsic)
  • 3rd p-type region is heavily doped layer.

2
APD
  • The diode operates in the reverse bias mode in
    order to increase the field in the depletion
    regions.
  • Applying an adequate R.B. will force the
    depletion region in the p-layer to reach-through
    to layer.
  • The field ultimately extends from -side
    depletion layer to the - side depletion
    layer.
  • Absorption of photons and therefore
    photogeneration takes place in the long
    layer.
  • It is a uniform field in the layer due to the
    small net space charge density.

3
APD
  • The E-field is at a maximum at the - side
    and a minimum at the - side.
  • Drifting electrons arriving at the p-layer
    experience elevated fields and acquire enough
    kinetic energy (greater than Eg) to impact-ionize
    some of the Si covalent bonds and release EHPs.
  • These EHPs can be accelerated by high fields to
    high kinetic energies to cause further impact
    ionization releasing even more EHPs leading to an
    avalanche of impact-ionization process.

4
APD
  • In summary a single elctron entering the p-layer
    can generate a large number of EHPs which
    contribute to an observed photocurrent.
  • APDs have an internal gain mechanism.
  • This avalanche multiplication corresponds to a
    quantum efficiency greater than unity.
  • Why is photogeneration restricted to the
    region ?
  • Electrons as a carrier in Si have a higher impact
    ionization efficiency than holes (less excess
    noise in avalanche multiplied photocurrent).

5
APD
  • Factors determining speed
  • Time it takes for photogenerated electron to
    cross the absorption region ( layer) to the
    multiplication layer (p layer).
  • Time it takes for the avalanche process to
    build-up in the p-region and generate EHPs.
  • Time it takes for the last hole released in the
    avalanche process to vacate the region.

6
Avalanche Multiplication Factor
7
APD
  • Response time of APD is longer than PIN diode
    however it offers gain.
  • APD does not require additional amplification
    which introduces delay to PIN diode.
  • Drawback of APD The peripheral edge of the
    p junction reaches avalanche breakdown before
    the p window of illumination area.
  • Uniform avalanche multiplication is required to
    promote avalanching of primary photocurrent
    versus dark current (generates random EHPs).
    Remedy guard ring.

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