Optical transmission system with a receiver using full optical clock recovery

The present invention relates to an optical transmission system comprising a transmitter for transmitting optical pulses via an optical transmission medium to a receiver, the receiver comprises optical clock recovery means for generating a sequence of optical pulses with a frequency related to a pul...

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Bibliographische Detailangaben
Hauptverfasser: Smets, Robert C. J, Reid, John J. E
Format: Patent
Sprache:eng
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Beschreibung
Zusammenfassung:The present invention relates to an optical transmission system comprising a transmitter for transmitting optical pulses via an optical transmission medium to a receiver, the receiver comprises optical clock recovery means for generating a sequence of optical pulses with a frequency related to a pulse frequency of the optical pulses received from the transmission medium, the optical clock recovery means comprises an optical amplifier having its input coupled to its output via a feedback loop, said feedback loop comprises a non linear element, the optical clock recovery means comprises injection means for injecting the optical signal received from the optical transmission medium. In an optical transmission system a transmitter () generates a sequence of time domain division multiplexed pulses and transmits them via an optical transmission medium () to a receiver (). In the receiver () the received optical multiplex signal is applied to an optical demultiplexer () and to a clock recovery element (). The clock recovery element () generates optical clock pulses which are used to control optically controlled optical switches () which demultiplex the optical signal. The optical clock recovery circuit is based on a laser which is mode locked by the received optical signal. The mode locked laser comprises an optical amplifier () having its output coupled to its input by a feedback loop comprising a polarization controller (), a saturable absorber (), a coupling element () and a adjustable delay (). The received optical signal is coupled into the feedback loop by means of the coupling element (). The saturable absorber () comprises a 3 dB, 90° coupling element () being coupled to a secondary loop. Said secondary loop comprises an attenuator () and an amplifier (). The amplifier () is placed asymmetrically in the secondary loop. Due to the non-linearity in the secondary loop, the optical pulses propagating in the secondary loop interfere destructively for low signal levels, and interfere constructively for high signal levels.