The coefficients from the polynomial fit to the dispersion profile do not have enough digits to reproduce the curve. A scaling error on Figs. 3 and 4 has been corrected.

©2005 Optical Society of America

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  1. T. V. Andersen, K. M. Hilligsøe, C. K. Nielsen, J. Thøgersen, K. P. Hansen, S. R. Keiding, and J. J. Larsen, “Continuous-wave wavelength conversion in a photonic crystal fiber with two zero-dispersion wavelengths,” Opt. Express 12, 4113–4122 (2004), http://www.opticsexpress.org/abstract.cfm?URI=OPEX-12-17-4113.
    [Crossref] [PubMed]

2004 (1)

Andersen, T. V.

Hansen, K. P.

Hilligsøe, K. M.

Keiding, S. R.

Larsen, J. J.

Nielsen, C. K.

Thøgersen, J.

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Figures (1)

Fig. 1.
Fig. 1.

Left: The scaled dispersion terms β 2, β 4, β 6 and β 8 as functions of λ. The higher order dispersion terms are of considerable size and change sign several times in the shown interval. Right: A zoom on the high-frequency ZDW shows that β 4 and β 8 are negative below the ZDW. They can therefore compensate for the positive β 2 and β 6 which means that phasematching is possible in the normal dispersion regime.