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Lecture III.
. Transient and Steady-state
Photoconductivity in
Insulators, Theory and
Experiment
Small-signal limit
Drift Mobility
Trapping (shallow and deep)
Transient photoconductivity-
determination of the drift mobility
For an applied electric field
constant in position and time,
E=V/d, where V is the applied
potential across the
photoconductor, and d its
thickness.
Let v be the drift velocity, and μ be
the carrier mobility, so, by
definition,
μ=v/E
When the carriers reach the back
electrode (x=d), time is their-time-
of-flight t.
Then μ= (d/t)/(V/d)
Carrier Trapping
Shallow Traps
Deep Traps
Lecture 3 oms
Lecture 3 oms
Lecture 3 oms
Lecture 3 oms
Lecture 3 oms
Lecture 3 oms
Lecture 3 oms
Lecture 3 oms
Lecture 3 oms

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Lecture 3 oms

  • 1. Lecture III. . Transient and Steady-state Photoconductivity in Insulators, Theory and Experiment Small-signal limit Drift Mobility Trapping (shallow and deep)
  • 3.
  • 4.
  • 5. For an applied electric field constant in position and time, E=V/d, where V is the applied potential across the photoconductor, and d its thickness.
  • 6. Let v be the drift velocity, and μ be the carrier mobility, so, by definition, μ=v/E When the carriers reach the back electrode (x=d), time is their-time- of-flight t. Then μ= (d/t)/(V/d)
  • 7.
  • 8.
  • 9.
  • 10.
  • 11.
  • 12.
  • 13.
  • 14.
  • 15.
  • 16.
  • 17.
  • 18.
  • 19.
  • 20.
  • 21.
  • 22.
  • 25.
  • 26.
  • 27.