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Highly nonlinear dispersion-flattened photonic crystal fibers for supercontinuum generation in a telecommunication window

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Abstract

We propose a new structure of highly nonlinear dispersion-flattened (HNDF) photonic crystal fiber (PCF) with nonlinear coefficient as large as 30 W-1km-1 at 1.55 μm designed by varying the diameters of the air-hole rings along the fiber radius. This innovative HNDF-PCF has a unique effective-index profile that can offer not only a large nonlinear coefficient but also flat dispersion slope and low leakage losses. It is shown through numerical results that the novel microstructured optical fiber with small normal group-velocity dispersion and nearly zero dispersion slope offers the possibility of efficient supercontinuum generation in the telecommunication window using a few ps pulses.

©2004 Optical Society of America

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Figures (4)

Fig. 1.
Fig. 1. Examples of PCFs and their effective refractive-index profiles. The air-hole diameters are (a) d 1 > d 2 = … = dn and (b) d 2 < d 1 = d 3 = … = dn .
Fig. 2.
Fig. 2. (a) Highly nonlinear dispersion-flattened PCF with ten air-hole rings and (b) its effective refractive-index profile. The hole-to-hole spacing is Λ = 0.89 μm and the air-hole diameters are d 1 = 0.41Λ, d 2 = 0.85Λ, d 3 = 0.92Λ, d 4 = 0.53Λ, d 5 = … = d 10 = 0.60Λ.
Fig. 3.
Fig. 3. (a) Chromatic dispersion curve, (b) confinement loss, and (c) effective mode area as a function of wavelength for the HNDF-PCF with ten air-hole rings in Fig. 2(a).
Fig. 4.
Fig. 4. Evolution of (a) waveforms and (b) spectrums in HNDF-PCF.

Equations (1)

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A z + α 2 A + i 2 β 2 2 A T 2 1 6 β 3 3 A T 3 i 24 β 4 4 A T 4 = i γ [ A 2 A + i λ c 2 π c T ( A 2 A ) T R A A 2 T ] ,
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