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White-light supercontinuum generation in normally dispersive optical fiber using original multi-wavelength pumping system

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Abstract

We report on the experimental demonstration of a white-light supercontinuum generation in normally dispersive singlemode air-silica microstructured fiber. We demonstrate that the simultaneous excitation of the microstuctured fiber in its normal and anomalous dispersion regimes using the fundamental and second harmonic signals of a passively Q-switched microchip laser leads to a homogeneous supercontinuum in the visible range. This pumping scheme allows the suppression of the cascaded Raman effect predominance in favor of an efficient spectrum broadening induced by parametric phenomena. A flat supercontinuum extended from 400 to 700 nm is achieved.

©2004 Optical Society of America

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Figures (6)

Fig. 1.
Fig. 1. Experimental set-up and cross sectional scanning electron microscope image of the microstructured air-silica fiber.
Fig. 2.
Fig. 2. Computed chromatic dispersion (a) and effective area (b) of the fundamental mode of the microstructured fiber versus the wavelength. Inset: transverse energy distribution calculated at λ = 800 nm.
Fig. 3.
Fig. 3. Continuum generation in normal dispersion regime in the case of single (a) and dual (b) pump configuration. Pictures: diffracted beams. Graph: corresponding recorded power spectra. (a) The cascaded Raman effect is clearly visible in the presence of a single pump (532 nm). (b) The spectrum smoothly and symmetrically broadens when a second pump (1064 nm) is added. The corresponding singlemode transverse energy distribution is shown in inset (far field pattern).
Fig. 4.
Fig. 4. Continuum power spectrum measured in the infrared range (anomalous dispersion regime).
Fig. 5.
Fig. 5. Continuum power spectrum obtained in the visible range when using both 532 and 1064 nm pumps, but for an insufficient value of ratio Pω/P.
Fig. 6.
Fig. 6. Infrared continuum power spectrum obtained in a microstructured fiber fabricated at IRCOM with non flame fused silica glass. No more OH- absorption peak is observable at 1400 nm.
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