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Experimental demonstration of wavelength conversion between ps-pulses based on cascaded sum- and difference frequency generation (SFG+DFG) in LiNbO3 waveguides

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Abstract

All-optical wavelength conversion between ps-pulses based on cascaded sum- and difference frequency generation (SFG+DFG) is proposed and experimentally demonstrated in periodically poled LiNbO3 (PPLN) waveguides. The signal pulse with 40-GHz repetition rate and 1.57-ps pulse width is adopted. The converted idler wavelength can be tuned from 1527.4 to 1540.5nm as the signal wavelength is varied from 1561.9 to 1548.4nm. No obvious changes of the pulse shape and width, also no chirp are observed in the converted idler pulse. The results imply that single-to-multiple channel wavelength conversions can be achieved by appropriately tuning the two pump wavelengths.

©2005 Optical Society of America

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Figures (10)

Fig. 1.
Fig. 1. Experimental setup for SFG+DFG based wavelength conversion between ps-pulses; PC: polarization controller, ATT: attenuator, TF: tunable filter, OSA: optical spectrum analyzer, CSA: communication signal analyzer.
Fig. 2.
Fig. 2. Measured output spectrum from the SFG+DFG based wavelength converter. Two pump wavelengths are 1540.9 and 1549.1nm respectively and the signal wavelength is tuned at 1555.9nm.
Fig. 3.
Fig. 3. Measured output spectra from the SFG+DFG based wavelength converter for the different signal wavelengths: (a) 1555.3nm, (b) 1561.9nm. Two pump wavelengths are kept at 1540.9 and 1549.1nm respectively during the experiments.
Fig. 4.
Fig. 4. Conversion efficiency vs. initial signal wavelength. Two pump wavelengths are kept at 1540.9 and 1549.1nm respectively and the pump powers are both about 10dBm during the experiments.
Fig. 5.
Fig. 5. Measured output spectra from the SFG+DFG based wavelength converter with two pump wavelength difference |λ P1 -λ P2| changed: (a) 17.3nm, (b) 2.3nm. Signal wavelength is kept at 1561.9nm and the idler wavelength is at about 1528.5nm during the experiments.
Fig. 6.
Fig. 6. Conversion efficiency vs. the difference of the two pump wavelengths. Signal wavelength is kept at 1561.9nm and the idler wavelength is at about 1528.5nm during the experiments. The two pump powers are chosen both at about 10dBm.
Fig. 7.
Fig. 7. Conversion efficiency vs. wavelength detuning of pump1 when pump2 is fixed at 1549.1nm. Signal wavelength is kept at 1556.6nm and the idler wavelength is varied as pump1 wavelength is tuned. The two pump powers are chosen both at about 10dBm. (λ P10 = 1540.9nm).
Fig. 8.
Fig. 8. Measured output spectrum from the SFG+DFG based wavelength converter with pump2 fixed at 1549.1nm and pump1 tuned at 1545.0nm. Signal wavelength is kept at 1556.6nm.
Fig. 9.
Fig. 9. Variations of the measured pulse duration (unclosed circles) and spectrum bandwidth of the converted idler pulses (unclosed squares).
Fig. 10.
Fig. 10. Variations of the duration-bandwidth product of the converted idler pulses. The dashed line represents the transform limited case for hyperbolic-secant pulse as a reference.
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