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All-optical modulation format conversion from on-off-keying to multiple-level phase-shift-keying based on nonlinearity in optical fiber

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Abstract

We propose an all-optical modulation format conversion scheme from non-return-to-zero on-off-keying (NRZ-OOK) to return-to-zero (RZ) multiple-level phase-shift-keying (PSK) based on nonlinearity in optical fiber. The proposed conversion scheme is numerically investigated and experimentally demonstrated. We experimentally demonstrate error-free operation of NRZ-OOK/RZ- binary PSK conversion at 10.7 Gb/s. The operation of the NRZ-OOK/RZ-quadrature PSK conversion is shown by eye opening after balanced receiving at a symbol rate of 10.7 Gsymbol/s. In addition, we demonstrate the feasibility of the modulation format conversion from NRZ-OOK to RZ-8-levels PSK by numerical simulation.

©2007 Optical Society of America

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Figures (13)

Fig. 1.
Fig. 1. All-optical modulation format conversion at the gateway node between MAN and WAN.
Fig. 2.
Fig. 2. Schematic diagram of the proposed modulation format conversion.
Fig. 3.
Fig. 3. The probe pulse after passing through HNLF: (a) Waveform; (b) Phase.
Fig. 4.
Fig. 4. Experimental setup for NRZ-OOK/RZ-BPSK conversion.
Fig. 5.
Fig. 5. Eye diagram and spectrum of converted signal before 1-bit delay interferometer: (a) Eye diagram; (b) Spectrum.
Fig. 6.
Fig. 6. Eye diagrams of converted signal after 1-bit delay interferometer: (a) Constructive output; (b) Destructive output.
Fig. 7.
Fig. 7. Eye diagrams after the balanced receiver.
Fig. 8.
Fig. 8. Measured BER.
Fig. 9.
Fig. 9. The probe pulse after passing through HNLF: (a) Waveform; (b) Phase.
Fig. 10.
Fig. 10. Experimental setup for NRZ-OOK/RZ-QPSK conversion.
Fig. 11.
Fig. 11. Eye diagram and spectrum of converted signal before 1-bit delay interferometer: (a) Eye diagram; (b) Spectrum.
Fig. 12.
Fig. 12. Eye diagrams of converted signal after 1-bit delay interferometer: (a) Constructive output; (b) Destructive output; (c) Received signal with balanced receiver.
Fig. 13.
Fig. 13. The probe pulse after passing through HNLF: (a) Waveform; (b) Phase.

Tables (1)

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Table 1. Parameters of the HNLF @1550 nm.

Equations (2)

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Δ ϕ pro = k = 1 K Δ ϕ k = 2 γ L eff k = 1 K P k ,
i E z β 2 2 2 E t 2 + s E 2 E = iγE .
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