Abstract

An error was made in the calculation of the relative intensity noise (RIN) because of an incorrectly specified value of the photodetector DC transimpedance gain.

© 2012 Optical Society of America

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References

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  1. U. Møller, S. T. Sørensen, C. Jakobsen, J. Johansen, P. M. Moselund, C. L. Thomsen, and O. Bang, “Power dependence of supercontinuum noise in uniform and tapered PCFs,” Opt. Express 20, 2851–2857 (2012).
    [Crossref] [PubMed]
  2. U. Møller, S. T. Sørensen, C. Larsen, P. M. Moselund, C. Jakobsen, J. Johansen, C. L. Thomsen, and O. Bang, “Optimum PCF tapers for blue-enhanced supercontinuum sources,” Opt. Fiber Technol. (2012), (article in press) http://dx.doi.org/10.1016/j.yofte.2012.07.010 .
    [Crossref]

2012 (1)

Bang, O.

Jakobsen, C.

Johansen, J.

Møller, U.

Moselund, P. M.

Sørensen, S. T.

Thomsen, C. L.

Opt. Express (1)

Other (1)

U. Møller, S. T. Sørensen, C. Larsen, P. M. Moselund, C. Jakobsen, J. Johansen, C. L. Thomsen, and O. Bang, “Optimum PCF tapers for blue-enhanced supercontinuum sources,” Opt. Fiber Technol. (2012), (article in press) http://dx.doi.org/10.1016/j.yofte.2012.07.010 .
[Crossref]

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Figures (3)

Fig. 3
Fig. 3

RIN vs. input power and wavelength in (a) the uniform fiber and (b) the tapered fiber. The thick black line shows the spectral edges. The dots show the measurement points.

Fig. 4
Fig. 4

RIN of the uniform (black squares) and the tapered fiber (red circles) (a) vs. wavelength at fixed input power of 0.55 W (open symbols) and 10 W (solid symbols) and (b) vs. input power at fixed wavelength of 550 nm (open symbols) and 1100 nm (solid symbols).

Fig. 5
Fig. 5

RIN at the spectral (a) blue and (b) red edge of the uniform and tapered fiber, respectively, as a function of wavelength.

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