Abstract

Using femtosecond upconversion we investigate the time and wavelength structure of infrared supercontinuum generation. It is shown that radiation is scattered into higher order spatial modes (HOMs) when generating a supercontinuum using fibers that are not single-moded, such as a step-index ZBLAN fiber. As a consequence of intermodal scattering and the difference in group velocity for the modes, the supercontinuum splits up spatially and temporally. Experimental results indicate that a significant part of the radiation propagates in HOMs. Conventional simulations of super-continuum generation do not include scattering into HOMs, and including this provides an extra degree of freedom for tailoring supercontinuum sources.

Highlights

  • Supercontinuum generation has been a field of great interest, and the physical processes involved in the generation have been studied vigorously

  • Numerous applications have emerged since the first supercontinuum in bulk glass was reported by Alfano et al [2], in such diverse fields as spectroscopy [3, 4] and optical metrology [5, 6]

  • Simulations are carried out using the multi-mode variant of the generalized nonlinear Schrodinger equation (GNLSE) (MM-GNLSE) in [18]

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Summary

Introduction

Supercontinuum generation has been a field of great interest, and the physical processes involved in the generation have been studied vigorously (for a review, see [1]). Supercontinua have been pushed into the mid-infrared, making room for new applications in spectroscopy and microspectroscopy [7,8,9,10], as the molecular fingerprint region can be reached. Novel soft glass fibers such as ZBLAN or chalcogenide are often used to be able to reach into the mid-infrared. ZBLAN fibers are not microstructured and to develop new fibers optimized for supercontinua generation, it is important to consider the generation process correctly. The normalized frequency parameter V determines the number of modes that can propagate through the fiber at a given wavelength, and for step-index fibers, V is defined as [11]

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