Abstract

We demonstrate real-time transmission of 16 Tb/s (80x200Gb/s) over 1020km TeraWave ULL fiber with 170km span length using the world’s first 200Gb/s CFP2-DCO module with a record low power consumption less than 0.1W/Gbps.

© 2018 Optical Society of America under the terms of the OSA Open Access Publishing Agreement

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References

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  1. http://www.tmcnet.com/tmc/whitepapers/documents/whitepapers/2013/9378-bell-labs-metro-network-traffic-growth-an-architecture.pdf
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  3. http://www.oiforum.com/public/documents/OIF-MSA-100GLH-EM-01.0.pdf
  4. C. R. Doerr, “Photonic Integrated Circuits for High-Speed Communications,” presented at the 2010 Conference on Lasers and Electro-Optics (CLEO) and Quantum Electronics and Laser Conference (QELS), San Jose, California, 16–21 May 2010, CFE3.
    [Crossref]
  5. J. C. Geyer, C. Rasmussen, B. Sha, T. Nielsen, and M. Givehchi, “Power Efficient Coherent Transceivers,” presented at the 42nd European Conference on Optical Communication (ECOC), Dusseldorf, Germany, 18–22 Sept. 2016, P109.
  6. C. Rasmussen, “Power and Reach Trade-offs Increasing the Optical Channel Rate Through Higher Baud Rate and Modulation Order,” in Optical Fiber Communication Conference, OSA Technical Digest (online) (Optical Society of America, 2017), paper Th3G.1.
    [Crossref]
  7. http://www.lightwaveonline.com/articles/2016/11/osfp-msa-targets-400-gbps-optical-transceiver-module.html
  8. http://www.lightwaveonline.com/articles/2016/03/qsfp-dd-msa-targets-200g-400g-optical-transceivers.html
  9. http://www.gazettabyte.com/home/2017/6/22/the-oifs-400zr-coherent-interface-starts-to-take-shape.html
  10. P. Poggiolini, “The GN Model of Non-Linear Propagation in Uncompensated Coherent Optical Systems,” J. Lightwave Tech. 30(24), 3857–3879 (2012).
    [Crossref]

2012 (1)

P. Poggiolini, “The GN Model of Non-Linear Propagation in Uncompensated Coherent Optical Systems,” J. Lightwave Tech. 30(24), 3857–3879 (2012).
[Crossref]

Poggiolini, P.

P. Poggiolini, “The GN Model of Non-Linear Propagation in Uncompensated Coherent Optical Systems,” J. Lightwave Tech. 30(24), 3857–3879 (2012).
[Crossref]

J. Lightwave Tech. (1)

P. Poggiolini, “The GN Model of Non-Linear Propagation in Uncompensated Coherent Optical Systems,” J. Lightwave Tech. 30(24), 3857–3879 (2012).
[Crossref]

Other (9)

http://www.tmcnet.com/tmc/whitepapers/documents/whitepapers/2013/9378-bell-labs-metro-network-traffic-growth-an-architecture.pdf

http://www.ecocexhibition.com/sites/default/files/file/Market%20Focus%20Presentations%202012/Acacia%20ECOC%202012.pdf

http://www.oiforum.com/public/documents/OIF-MSA-100GLH-EM-01.0.pdf

C. R. Doerr, “Photonic Integrated Circuits for High-Speed Communications,” presented at the 2010 Conference on Lasers and Electro-Optics (CLEO) and Quantum Electronics and Laser Conference (QELS), San Jose, California, 16–21 May 2010, CFE3.
[Crossref]

J. C. Geyer, C. Rasmussen, B. Sha, T. Nielsen, and M. Givehchi, “Power Efficient Coherent Transceivers,” presented at the 42nd European Conference on Optical Communication (ECOC), Dusseldorf, Germany, 18–22 Sept. 2016, P109.

C. Rasmussen, “Power and Reach Trade-offs Increasing the Optical Channel Rate Through Higher Baud Rate and Modulation Order,” in Optical Fiber Communication Conference, OSA Technical Digest (online) (Optical Society of America, 2017), paper Th3G.1.
[Crossref]

http://www.lightwaveonline.com/articles/2016/11/osfp-msa-targets-400-gbps-optical-transceiver-module.html

http://www.lightwaveonline.com/articles/2016/03/qsfp-dd-msa-targets-200g-400g-optical-transceivers.html

http://www.gazettabyte.com/home/2017/6/22/the-oifs-400zr-coherent-interface-starts-to-take-shape.html

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Figures (7)

Fig. 1
Fig. 1 Transceiver module landscape (Ref [2].).
Fig. 2
Fig. 2 Evolution in power and density per 100Gbps for coherent transceiver modules.
Fig. 3
Fig. 3 Circulating loop setup for transmission experiments.
Fig. 4
Fig. 4 PM-8QAM and PM-16QAM pre-emphasis measurement at 4 bits/s/Hz and 5.33 bits/s/Hz SE in back-to-back and transmission.
Fig. 5
Fig. 5 Measured OSNR and Q2-factor performance across 80 channels at 50GHz channel spacing after 1020 km.
Fig. 6
Fig. 6 Left: Optical spectrum of PM-8QAM after 50GHz demuxer w/o frequency detuning. Right: Performance penalty with frequency detuning after 1020km.
Fig. 7
Fig. 7 Long term measurement of PM-16QAM at 37.5 GHz channel spacing.

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