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Measurement of co- and cross-polarized Raman spectra in silica fiber for small detunings: erratum

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Abstract

We present corrected versions of Fig. 5(a) and Fig. 6(b) below with the original captions.

©2005 Optical Society of America

In our recent paper [1], a spurious data point was erroneously included in Fig. 5(a) and the scaling of the s 1 axis in Fig. 6(b) was incorrectly represented. Figure 7, the main result of the paper, was correct.

In addition, a correction is needed in the 9th to last line of the text on page 2243. Here the expression “R g (ω p ,Ω)=35.8s 1” should have read “(1/2)R g (ω p ,Ω) =35.8s 1”.

 figure: Fig. 5.

Fig. 5. (a) Total detected photons at detuning 0.17 THz (black) and 0.47 THz (gray), respectively, as a function of the injected pump photons. Second-order polynomials, N a =s 1 N p +s 2 Np2 , are shown to fit the experimental data (dot-dashed line). The contributions of linear scattering, s 1 N p , (solid line) and quadratic scattering, s 2 Np2 , (dotted line) are plotted separately as well.

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 figure: Fig. 6.

Fig. 6. (b) Fitting parameter s 1 co-(solid squares) and cross-polarized (hollow squares) with the pump versus detuning.

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References and links

1. X. Li, P. L. Voss, J. Chen, K. F. Lee, and P. Kumar, “Measurement of co- and crosspolarized Raman spectra in silica fiber for small detunings,” Opt. Express 13, 2236–2244 (2005), http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-6-2236. [CrossRef]   [PubMed]  

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Figures (2)

Fig. 5.
Fig. 5. (a) Total detected photons at detuning 0.17 THz (black) and 0.47 THz (gray), respectively, as a function of the injected pump photons. Second-order polynomials, N a =s 1 N p +s 2 N p 2 , are shown to fit the experimental data (dot-dashed line). The contributions of linear scattering, s 1 N p , (solid line) and quadratic scattering, s 2 N p 2 , (dotted line) are plotted separately as well.
Fig. 6.
Fig. 6. (b) Fitting parameter s 1 co-(solid squares) and cross-polarized (hollow squares) with the pump versus detuning.
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