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book Optical Fiber Communications 4th Edition by Gerd Keiser cover

Optical Fiber Communications 4th Edition by Gerd Keiser

Edition 4ISBN: 978-0073380711
book Optical Fiber Communications 4th Edition by Gerd Keiser cover

Optical Fiber Communications 4th Edition by Gerd Keiser

Edition 4ISBN: 978-0073380711
Exercise 6
The low-frequency gain M 0 of an avalanche photodiode depends on the carrier ionization rate and on the width of the multiplication region, both of which depend on the applied reverse-bias voltage V a. This gain can be described by the empirical relationship 33 The low-frequency gain M 0 of an avalanche photodiode depends on the carrier ionization rate and on the width of the multiplication region, both of which depend on the applied reverse-bias voltage V a. This gain can be described by the empirical relationship 33   (P6.4) where V B is the breakdown voltage at which M 0 goes to infinity ( M 0 ), I M is the total multiplied current, and R M accounts for the photodiode series resistance and the detector load resistance. The exponential factor n depends on the semiconductor material and its doping profile. Its value varies between about 2.5 and 7. ( a ) Show that for applied voltages near the breakdown voltage, at which point V B » I M R M , Eq. (P6.4) can be approximated by    ( b ) The maximum value of M 0 occurs when V a = V B. Show that, at this point,  (P6.4)
where V B is the breakdown voltage at which M 0 goes to infinity ( M 0 ), I M is the total multiplied current, and R M accounts for the photodiode series resistance and the detector load resistance. The exponential factor n depends on the semiconductor material and its doping profile. Its value varies between about 2.5 and 7.
( a ) Show that for applied voltages near the breakdown voltage, at which point V B » I M R M , Eq. (P6.4) can be approximated by The low-frequency gain M 0 of an avalanche photodiode depends on the carrier ionization rate and on the width of the multiplication region, both of which depend on the applied reverse-bias voltage V a. This gain can be described by the empirical relationship 33   (P6.4) where V B is the breakdown voltage at which M 0 goes to infinity ( M 0 ), I M is the total multiplied current, and R M accounts for the photodiode series resistance and the detector load resistance. The exponential factor n depends on the semiconductor material and its doping profile. Its value varies between about 2.5 and 7. ( a ) Show that for applied voltages near the breakdown voltage, at which point V B » I M R M , Eq. (P6.4) can be approximated by    ( b ) The maximum value of M 0 occurs when V a = V B. Show that, at this point,
( b ) The maximum value of M 0 occurs when V a = V B. Show that, at this point, The low-frequency gain M 0 of an avalanche photodiode depends on the carrier ionization rate and on the width of the multiplication region, both of which depend on the applied reverse-bias voltage V a. This gain can be described by the empirical relationship 33   (P6.4) where V B is the breakdown voltage at which M 0 goes to infinity ( M 0 ), I M is the total multiplied current, and R M accounts for the photodiode series resistance and the detector load resistance. The exponential factor n depends on the semiconductor material and its doping profile. Its value varies between about 2.5 and 7. ( a ) Show that for applied voltages near the breakdown voltage, at which point V B » I M R M , Eq. (P6.4) can be approximated by    ( b ) The maximum value of M 0 occurs when V a = V B. Show that, at this point,
Explanation
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Optical Fiber Communications 4th Edition by Gerd Keiser
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