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Theoretical and experimental study of fundamental differences in the noise suppression of high-speed SOA-based all-optical switches

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Abstract

We identify a fundamental difference between the ASE noise filtering properties of different all-optical SOA-based switch configurations, and divide the switches into two classes. An in-band ASE suppression ratio quantifying the difference is derived theoretically and the impact of the ASE filtering on the optical spectrum is verified experimentally using a hybrid DISC setup. ASE power suppression of around 3 dB over the total signal bandwidth is demonstrated.

©2005 Optical Society of America

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Figures (5)

Fig. 1.
Fig. 1. Schematics of (a) the DISC configuration and (b) the SOA-based MZI configuration.
Fig. 2.
Fig. 2. Normalized ASE power spectral density of SOA output (solid) and AMZI power transfer function (dashed) for τ=5 ps and Φ0=0.90π. Single-hatched area represents ASE power suppressed by AMZI.
Fig. 3.
Fig. 3. Experimental setup: Inline implementation of DISC
Fig. 4.
Fig. 4. (a) ASE spectra (resolution: 0.1 nm) at DISC output for TE/TM polarized ASE (solid/dashed), and for unpolarized ASE (dash-dotted). (b) Comparison of TE/TM ASE ratio (black squares) and ASE spectral fringe depth (white squares). Inset: detail of spectral fringe for I=150 mA.
Fig. 5.
Fig. 5. Optical probe spectra at DISC output with input polarizer (thick, solid) and without polarizer (thin, dashed) for an SOA bias of 150 mA and an AMZI phase bias of Φ0=0.90 π. Inset: Cross-correlation trace of switched probe.

Equations (4)

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H AMZ ( λ ) 2 = 1 2 [ 1 + cos ( 2 π λ λ P Δ λ τ + Φ 0 ) ]
IBSR 1 = 1 2 [ 1 + cos ( Φ 0 ) sinc ( π Δ λ F Δ λ τ ) ]
P ˜ DISC CQP ( λ ) = P ˜ ASE TE ( λ ) H AMZ TE ( λ ) 2 + P ˜ ASE TM ( λ ) H AMZ TM ( λ ) 2
= P ˜ SOA ( λ ) 2 [ 1 + ( 2 r 1 ) cos ( 2 π λ λ P Δ λ τ + Φ 0 ) ]
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