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Optical Receivers Theory and Operation

Optical Receivers Theory and Operation. Photodetector Requirements. High sensitivity ( responsivity ) at the desired wavelength and low responsivity elsewhere Low noise and reasonable cost Fast response time  high bandwidth Insensitive to temperature variations

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Optical Receivers Theory and Operation

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  1. Optical ReceiversTheory and Operation

  2. Photodetector Requirements • High sensitivity (responsivity) at the desired wavelength and low responsivity elsewhere • Low noise and reasonable cost • Fast response time  high bandwidth • Insensitive to temperature variations • Compatible physical dimensions • Long operating life

  3. Photodiodes • Due to above requirements, only photodiodes are used as photo detectors in optical communication systems • Positive-Intrinsic-Negative (pin) photodiode • No internal gain • Avalanche Photo Diode (APD) • An internal gain of M due to self multiplication • Photodiodes are reverse biased for normal operation

  4. Basic pin photodiode circuit • Incident photons trigger a photocurrent Ip in the external circuitry Photocurrent Incident Optical Power

  5. pin energy-band diagram Cut off wavelength depends on the bandgap energy

  6. Responsivity () Quantum Efficiency () = number of e-h pairs generated / number of incident photons Avalanche PD’s have an internal gain M mA/mW IM: average value of the total multiplied current M = 1 for PIN diodes

  7. Responsivity

  8. Signal to Noise Ratio Signal to noise Ratio (SNR) as a function of the average number of photo electrons per receiver resolution time for a photo diode receiver at two different values of the circuit noise Signal to noise Ratio (SNR) as a function of the average number of photoelectrons per receiver resolution time for a photo diode receiver and an APD receiver with mean gain G=100 and an excess noise factor F=2 At low photon fluxes the APD receiver has a better SNR. At high fluxes the photodiode receiver has lower noise

  9. Signal to Noise Ratio For high SNR • The Photodetector must have a large quantum efficiency (large responsivity or gain) to generate large signal current • Detector and amplifier noise must be low SNR Can NOT be improved by amplification

  10. Quantum (Shot Noise) Due optical power fluctuation because light is made up of discrete number of photons F(M): APD Noise Figure F(M) ~= Mx (0 ≤ x ≤ 1) Ip: Mean Detected Current B = Bandwidth

  11. Dark/Leakage Current Noise There will be some (dark and leakage ) current without any incident light. This current generates two types of noise Bulk Dark Current Noise ID: Dark Current Surface Leakage Current Noise (not multiplied by M) IL: Leakage Current

  12. Thermal Noise The photodetector load resistor RLcontributes a mean-square thermal (Johnson) noise current KB: Boltzmann’s constant = 1.38054 X 10(-23) J/K T is the absolute Temperature • Quantum and Thermal are the important noise • mechanisms in all optical receivers • RIN (Relative Intensity Noise) will also appear in analog • links

  13. Signal to Noise Ratio Detected current = AC component (ip) + DC component (Ip) Signal Power = <ip2>M2 Typically not all the noise terms will have equal weight

  14. SNR Dark current and surface leakage current noise are typically negligible, If thermal noise is also negligible For analog links, (RIN= Relative Intensity Noise)

  15. Response Time in pin photodiode Transit time, td and carrier drift velocity vd are related by For a high speed Si PD, td = 0.1 ns

  16. Rise and fall times • Photodiode has uneven rise and fall times depending on: • Absorption coefficient s() and • Junction Capacitance Cj

  17. Junction Capacitance εo = 8.8542 x 10(-12) F/m; free space permittivity εr = the semiconductor dielectric constant A = the diffusion layer (photo sensitive) area w = width of the depletion layer Large area photo detectors have large junction capacitance hence small bandwidth (low speed)  A concern in free space optical receivers

  18. Various pulse responses Absorbed optical power at distance x exponentially decays depending ons

  19. Digital Receiver Performance Probability of error assuming Equal ones and zeros Where, Depends on the noise variance at on/off levels and the Threshold voltage Vththat is decided to minimize the Pe Question: Do you think Vth = ½ [Von + Voff] ?

  20. Logic 0 and 1 probability distributions Asymmetric distributions Select Vth to minimize Pe

  21. Noise variances Probability of error depends on Vth and noise power

  22. Bit Error Rate BER is equal to number of errors divided by total number of pulses (ones and zeros). Total number of pulses is bit rate B times time interval. BER is thus not really a rate, but a unitless probability.

  23. Q Factor and BER

  24. BER vs. Q, continued When off = on and Voff=0 so that Vth=V/2, then Q=V/2. In this case,

  25. Fig. 7-7: BER (Pe) versus Q factor

  26. BER vs SNR(equal standard deviations and boff = 0)

  27. Sensitivity The minimum optical power that still gives a bit error rate of 10-9 or below

  28. Receiver Sensitivity (Smith and Personick 1982)

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