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Optical temporal encoding/decoding of short pulses using cascaded long-period fiber gratings

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Abstract

A novel, optical temporal encoding/decoding method is proposed and demonstrated. This can be accomplished by passing a short optical pulse through cascaded long-period fiber gratings. It has the advantages of constructing ultrafast codes and developing resistance to interferometric perturbations among the coded pulses. To verify the feasibility as a code generator, two types of codes are generated and compared with the predicted code patterns. In addition, to show an application for an optical code-division-multiplexing system, decoding performances with matched and unmatched decoders are compared.

©2003 Optical Society of America

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Figures (5)

Fig. 1.
Fig. 1. Schematic diagram of a temporal encoder using cascaded LPGs. Inset figures are the measured near-field patterns of the core mode and the cladding mode.
Fig. 2.
Fig. 2. The configurations and temporal responses of cascaded LPGs for two codes: C1 and C2.; (a) Structure of cascaded LPGs with C1; (b) Predicted response of cascaded LPGs with C1; (c) Measured response of cascaded LPGs with C1; (d) Structure of cascaded LPGs with C2; (e) Predicted response of cascaded LPGs with C2 (f) Measured response of cascaded LPGs with C2
Fig. 3.
Fig. 3. Transmission spectra of two cascaded LPGs with (a) C1 (b) C2. Inset figures are the predicted spectra.
Fig. 4.
Fig. 4. Experimental set-up. The first LPGs encode an input short pulse into C1, which is decoded by two cascaded LPGs with C1 (autocorrelation) and C2 (cross-correlation). EDFA is an erbium-doped fiber amplifier.
Fig. 5.
Fig. 5. Decoded signals obtained with (a) the matched decoder; C1*C1 (b) the unmatched decoder; C1*C2. Dotted line: predicted, solid line: measured. Inset figures are the predicted pulse trains measured after the decoder, but before the autocorrelator.

Equations (2)

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( β co β cl ) = 2 π Λ
Δ T = L c Δ m eff
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