Longitudinally thickness-controlled nanofilms on exposed core fibres enabling spectrally flattened supercontinuum generation

Longitudinally thickness-controlled nanofilms on exposed core fibres enabling spectrally flattened supercontinuum generation
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DOI:
10.37188/lam.2021.021
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发表时间:
2021
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通讯作者:
Tilman A. K. Lühder;H. Schneidewind;Erik P. Schartner;Heike Ebendorf-Heidepriem;M. A. Schmidt
Tilman A. K. Lühder;H. Schneidewind;Erik P. Schartner;Heike Ebendorf-Heidepriem;M. A. Schmidt
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作者:
Tilman A. K. Lühder;H. Schneidewind;Erik P. Schartner;Heike Ebendorf-Heidepriem;M. A. Schmidt

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Nonlinear frequency conversion is a pathway to unlock undiscovered physics and implement tailored light sources for spectroscopy or medicine. A key challenge is the establishment of spectrally flat outputs, which is particularly demanding in the context of soliton-based light conversion at low pump energy. Here, we introduce the concept of controlling nonlinear frequency conversion by longitudinally varying resonances, allowing the shaping of soliton dynamics and achieving broadband spectra with substantial spectral flatness. Longitudinally varying resonances are realised by nanofilms with gradually changing thicknesses located on the core of an advanced microstructured fibre. Nanofilms with engineered thickness profiles are fabricated by tilted deposition, representing a waveguide-compatible approach to nano-fabrication, and inducing wellcontrolled resonances into the system, allowing unique dispersion control along the fibre length. Key features and dependencies are examined experimentally, showing improved bandwidth and spectral flatness via multiple dispersive wave generation and dispersion-assisted soliton Raman shifts while maintaining excellent pulse-to-pulse stability and coherence in simulations, suggesting the relevance of our findings for basic science as well as tailored light sources. Introduction Broadband nonlinear light sources with specific spectral properties are essential for many applications such as metrology, optical coherence tomography, and spectroscopy. Within the context of nonlinear frequency conversion, one successful approach is the soliton-based supercontinuum generation (SCG), which relies on the fission of higher-order solitons and the associated emission of dispersive waves (DWs). Because of the long light/matter interaction lengths and strong mode confinement, this SCG scheme is highly effective in waveguides, particularly in optical fibres. It relies heavily on the dispersive properties of the underlying waveguide, suggesting a pathway for tailoring the light generation process through waveguide engineering. One essential challenge in current supercontinuum (SC) research is the design of ultrafast soliton-based sources with a flat output spectrum, that is, with a flat power spectral density across defined spectral intervals. Spectral flatness is required, for example, to provide high quality point spread functions in optical coherence tomography and for handheld spectroscopic devices that cannot provide high dynamic ranges compared to modern heavy laboratory equipment. Using long pulse lengths or high pulse energies is an alternative method to obtain flat broadband spectra through modulation instability. However, this is directly associated with the pulse-to-pulse fluctuations of the output spectrum and the associated loss of coherence. Here, one promising Correspondence: Markus Schmidt (markus-alexander.schmidt@uni-jena.de) Leibniz Institute of Photonic Technology, Albert-Einstein-Str. 9, 07745 Jena, Germany School of Physical Sciences and ARC Centre of Excellence for Nanoscale BioPhotonics (CNBP) and Institute for Photonics and Advanced Sensing (IPAS), The University of Adelaide, Adelaide SA 5005, Australia Otto Schott Institute of Material Research, Fraunhoferstr. 6, 07743 Jena, Germany Abbe School of Photonics and Physics Faculty, Friedrich Schiller University, 07743 Jena, Germany pathway to spectrally homogenise the output at low input energy without using modulation instability relies on longitudinally modulating the dispersion of the waveguide by geometrically changing the waveguide cross section along its axis, leading to effects such as multiple DW emission. Both cascaded step-wise, discreetly changing the dispersion profiles via spliced fibre sections; furthermore, continuously (smoothly) varying dispersion landscapes have been realised in systems such as tapered photonic © The Author(s) 2021 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution, and reproduction. in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third-party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, permission will be obtained directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/ ACCEPTED ARTICLE PREVIEW