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Continuous-wave wavelength conversion in a photonic crystal fiber with two zero-dispersion wavelengths: erratum

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Abstract

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

In the article[1] we showed the measured dispersion profile of a photonic crystal fiber with two zero dispersion wavelengths. Coefficients from a 9th order polynomial fit to this dispersion curve were listed in Table 1. Unfortunately the number of digits shown in the table is not sufficient to reproduce the curve-we have found that the coefficients must have 10 digits for the expansion to be accurate. Information about the dispersion profile can be obtained by contacting the authors.

The Figs. 3 and 4 show scaled higher order terms of the dispersion. The curves have been scaled to f s 2/mm while the units on the vertical axes are f s 2/cm. In the following figures the scaling has been corrected to match the units f s 2/cm.

 figure: 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.

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References and links

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]  

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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.
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