Optical Receivers
MEC
Contents
• Digital Optical Fiber Receiver.
• Equalizer.
• Amplifier Configurations
- Low-impedance Front-end.
- High-impedance Front-end.
- Transimpedance Front-end.
• Comparison
Digital Optical Fiber Receiver
• Optical detector represented as a current
source idet.
• Noise sources - it, iTS and iamp , amplifier
and equalizer follows.
• Equalization compensates for signal
distortion due to combined transmitter,
medium and receiver characteristics.
Digital Optical Fiber Receiver
Equivalent Circuit
Equalizer
• Equalizer a frequency-shaping filter,
frequency response inverse of overall
system frequency response.
• Boost high-frequency components, correct
overall amplitude of frequency response.
• To acquire desired spectral shape & to
minimize intersymbol interference, system
phase frequency response to be linear.
Equalizer
• Applies selective
phase shifts to
particular frequency
components.
• Minimize noise
contributions from the
sources, maximize
receiver sensitivity,
maintain a suitable
bandwidth.
Amplifier Configurations
• Basic amplifier
configurations:
- Low-impedance
front-end.
- High-impedance
(integrating) front-
end.
- Transimpedance
front-end.
Low-impedance Front-end Amplifier
• Voltage amplifier
with effective input
resistance Ra.
• Detector loaded with
a bias resistor Rb
and an amplifier.
• Bandwidth
determined by
passive impedance
across detector
terminals (RL).
Modified total load
resistance
Low-impedance Front-end Amplifier
• RL may be modified to incorporate the
parallel resistance of detector bias
resistor Rb and amplifier input resistance
Ra.
• To achieve optimum bandwidth, Rb and Ra
to be minimized - low-impedance front-end
design.
• Design allows thermal noise to dominate
within the receiver, limits sensitivity.
Low-impedance Front-end Amplifier
• Trade-off between bandwidth and
sensitivity.
• Impractical for long-haul, wideband optical
fiber communication systems.
High-impedance (integrating)
Front-end Amplifier
• High i/p impedance
amplifier together
with a large detector
bias resistor to
reduce the effect of
thermal noise.
• Degraded frequency
response, bandwidth
relationship not
maintained for
wideband operation.
High-impedance (integrating)
Front-end Amplifier
• Detector output effectively integrated over
a large time constant, must be restored by
differentiation.
• Correct equalization required.
• Improvement in sensitivity over low-
impedance front-end design, creates a
heavy demand for equalization, limited
dynamic range.
High-impedance (integrating)
Front-end Amplifier
• Limitations on dynamic range result from
attenuation of the low-frequency signal
components by equalization, causes
amplifier to saturate at high signal levels.
• Amplifier saturates before equalization,
signal is heavily distorted.
• Reduction in dynamic range depends on
the amount of integration and subsequent
equalization employed.
Transimpedance Front-end
Amplifier
• Overcomes drawbacks of high-impedance
front end.
• Low-noise, high-input-impedance amplifier
with negative feedback.
• Operates as current mode amplifier, high
input impedance reduced by negative
feedback.
Transimpedance Front-end
Amplifier
Transimpedance Front-end
Amplifier
• Open loop current to voltage transfer
function HOL (ω)
G - open loop voltage gain of the
amplifier, ω - angular frequency of input.
Transimpedance Front-end
Amplifier
• Closed loop current to voltage transfer
function HCL(ω) (Rf - feedback resistor):
• Permitted electrical bandwidth (without
equalization)
Transimpedance Front-end
Amplifier
• Greater bandwidth than amplifiers without
feedback.
• When Rf << RTL, major noise contribution
is from thermal noise generated in Rf.
• Noise performance improved when Rf is
large.
• When Rf = RTL, noise performance
approaches that of high-impedance front
end.
Transimpedance Front-end
Amplifier
• Rf cannot be increased indefinitely due to
problems of stability with closed loop
design.
• Increasing Rf reduces bandwidth.
• Make G as large as the stability of closed
loop permits.
• Noise in transimpedance amplifier exceed
that incurred by high-impedance front-end
structure.
Transimpedance Front-end
Amplifier
• Greater bandwidth without equalization
than high-impedance front-end, but offset
by 13 dB noise penalty incurred.
• Optimized for noise performance at the
expense of bandwidth.
• Improvement in noise performance over
low-impedance front-end structures.
• Greater dynamic range.
Transimpedance Front-end
Amplifier
• Different attenuation mechanism for low
frequency components of the signal.
• Attenuation through negative feedback, low
frequency components amplified by device
closed loop rather than open loop gain.
• Improvement in dynamic range equal to
ratio of open loop to closed loop gains.
• Used in wideband optical fiber
communication receivers.
Thank You

Optical receivers

  • 1.
  • 2.
    Contents • Digital OpticalFiber Receiver. • Equalizer. • Amplifier Configurations - Low-impedance Front-end. - High-impedance Front-end. - Transimpedance Front-end. • Comparison
  • 3.
    Digital Optical FiberReceiver • Optical detector represented as a current source idet. • Noise sources - it, iTS and iamp , amplifier and equalizer follows. • Equalization compensates for signal distortion due to combined transmitter, medium and receiver characteristics.
  • 4.
    Digital Optical FiberReceiver Equivalent Circuit
  • 5.
    Equalizer • Equalizer afrequency-shaping filter, frequency response inverse of overall system frequency response. • Boost high-frequency components, correct overall amplitude of frequency response. • To acquire desired spectral shape & to minimize intersymbol interference, system phase frequency response to be linear.
  • 6.
    Equalizer • Applies selective phaseshifts to particular frequency components. • Minimize noise contributions from the sources, maximize receiver sensitivity, maintain a suitable bandwidth.
  • 7.
    Amplifier Configurations • Basicamplifier configurations: - Low-impedance front-end. - High-impedance (integrating) front- end. - Transimpedance front-end.
  • 8.
    Low-impedance Front-end Amplifier •Voltage amplifier with effective input resistance Ra. • Detector loaded with a bias resistor Rb and an amplifier. • Bandwidth determined by passive impedance across detector terminals (RL). Modified total load resistance
  • 9.
    Low-impedance Front-end Amplifier •RL may be modified to incorporate the parallel resistance of detector bias resistor Rb and amplifier input resistance Ra. • To achieve optimum bandwidth, Rb and Ra to be minimized - low-impedance front-end design. • Design allows thermal noise to dominate within the receiver, limits sensitivity.
  • 10.
    Low-impedance Front-end Amplifier •Trade-off between bandwidth and sensitivity. • Impractical for long-haul, wideband optical fiber communication systems.
  • 11.
    High-impedance (integrating) Front-end Amplifier •High i/p impedance amplifier together with a large detector bias resistor to reduce the effect of thermal noise. • Degraded frequency response, bandwidth relationship not maintained for wideband operation.
  • 12.
    High-impedance (integrating) Front-end Amplifier •Detector output effectively integrated over a large time constant, must be restored by differentiation. • Correct equalization required. • Improvement in sensitivity over low- impedance front-end design, creates a heavy demand for equalization, limited dynamic range.
  • 13.
    High-impedance (integrating) Front-end Amplifier •Limitations on dynamic range result from attenuation of the low-frequency signal components by equalization, causes amplifier to saturate at high signal levels. • Amplifier saturates before equalization, signal is heavily distorted. • Reduction in dynamic range depends on the amount of integration and subsequent equalization employed.
  • 14.
    Transimpedance Front-end Amplifier • Overcomesdrawbacks of high-impedance front end. • Low-noise, high-input-impedance amplifier with negative feedback. • Operates as current mode amplifier, high input impedance reduced by negative feedback.
  • 15.
  • 16.
    Transimpedance Front-end Amplifier • Openloop current to voltage transfer function HOL (ω) G - open loop voltage gain of the amplifier, ω - angular frequency of input.
  • 17.
    Transimpedance Front-end Amplifier • Closedloop current to voltage transfer function HCL(ω) (Rf - feedback resistor): • Permitted electrical bandwidth (without equalization)
  • 18.
    Transimpedance Front-end Amplifier • Greaterbandwidth than amplifiers without feedback. • When Rf << RTL, major noise contribution is from thermal noise generated in Rf. • Noise performance improved when Rf is large. • When Rf = RTL, noise performance approaches that of high-impedance front end.
  • 19.
    Transimpedance Front-end Amplifier • Rfcannot be increased indefinitely due to problems of stability with closed loop design. • Increasing Rf reduces bandwidth. • Make G as large as the stability of closed loop permits. • Noise in transimpedance amplifier exceed that incurred by high-impedance front-end structure.
  • 20.
    Transimpedance Front-end Amplifier • Greaterbandwidth without equalization than high-impedance front-end, but offset by 13 dB noise penalty incurred. • Optimized for noise performance at the expense of bandwidth. • Improvement in noise performance over low-impedance front-end structures. • Greater dynamic range.
  • 21.
    Transimpedance Front-end Amplifier • Differentattenuation mechanism for low frequency components of the signal. • Attenuation through negative feedback, low frequency components amplified by device closed loop rather than open loop gain. • Improvement in dynamic range equal to ratio of open loop to closed loop gains. • Used in wideband optical fiber communication receivers.
  • 22.