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Wide bandwidth slow light using a Raman fiber amplifier

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Abstract

We demonstrate an all-optical tunable pulse delay scheme that utilizes the power-dependent variation of the refractive index that accompanies stimulated Raman scattering in an optical fiber. Using this technique, we delay 430-fs pulses by up to 85% of a pulse width. The ability to accommodate the bandwidth of pulses shorter than 1 ps in a fiber-based system makes this technique potentially viable for producing controllable delays in ultra-high bandwidth telecommunication systems.

©2005 Optical Society of America

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Figures (5)

Fig. 1.
Fig. 1. The experimental setup used to demonstrate slow light in a Raman fiber amplifier (det, detector; FPC, fiber-polarization conroller; other abbreviations are described in the text). The reference pulse is used for the FTSI measurement of the signal delay.
Fig. 2.
Fig. 2. (a) Plots of gain versus pump peak power for several different signal wavelengths. (b) Gain slope versus signal-pump frequency detuning. The measured slopes plotted on the left axis are compared with the ASE spectrum which is plotted on the right axis.
Fig. 3.
Fig. 3. (a) Spectral interferograms along with the (b) Fourier-transformed pulse position.
Fig. 4.
Fig. 4. Plots of gain and delay vs. pump power.
Fig. 5.
Fig. 5. Amplitude of the transformed interferograms for pulse delay changes of 0 fs, 135 fs and 370 fs. The delay of 370 fs is the maximum delay achieved with our setup.

Equations (3)

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Δ T = G Γ ,
S ( ω ) = E 0 ( ω ) + E a ( ω ) 2
= E 0 ( ω ) 2 + E a ( ω ) 2 + 2 E 0 ( ω ) E a ( ω ) cos ( ϕ a ϕ 0 ) ,
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