Sune Dupont
Aarhus University
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Publication
Featured researches published by Sune Dupont.
Journal of The Optical Society of America B-optical Physics | 2012
Christian Agger; Christian Petersen; Sune Dupont; Henrik Steffensen; Jens Kristian Lyngsø; Carsten L. Thomsen; Jan Thøgersen; S. R. Keiding; Ole Bang
We present a detailed comparison between modeling and experiments on supercontinuum (SC) generation in a commercial ZBLAN step-index fiber. Special emphasis is put on identifying accurate material parameters by incorporating measurements of the ZBLAN Raman gain, fiber dispersion, and loss. This identification of accurate parameters is of great importance to substantiate numerical simulations of SC generation in soft-glass fibers. Good agreement between measurement and simulation is obtained when pumping both in the normal and anomalous dispersion regimes.
Optics Express | 2012
Sune Dupont; Christian Petersen; Jan Thøgersen; Christian Agger; Ole Bang; S. R. Keiding
Combining the molecular specificity of the infrared spectral region with high resolution microscopy has been pursued by researchers for decades. Here we demonstrate infrared supercontinuum radiated from an optical fiber as a promising new light source for infrared microspectroscopy. The supercontinuum light source has a high brightness and spans the infrared region from 1400 nm to 4000 nm. This combination allows contact free high resolution hyper spectral infrared microscopy. The microscope is demonstrated by imaging an oil/water sample with 20 μm resolution.
Proceedings of SPIE | 2012
Peter M. Moselund; Christian Rosenberg Petersen; Sune Dupont; Christian Agger; Ole Bang; S. R. Keiding
Based on the experience gained developing our market leading visible spectrum supercontinuum sources NKT Photonics has built the first mid-infrared supercontinuum source based on modelocked picosecond fiber lasers. The source is pumped by a ≈ 2 um laser based on a combination of erbium and thulium and use ZBLAN fibers to generate a 1.75-4.4 μm spectrum. We will present results obtained by applying the source for mid-infrared microscopy where absorption spectra can be used to identify the chemical nature of different parts of a sample. Subsequently, we discuss the possible application of a mid-IR supercontinuum source in other areas including infrared countermeasures.
Optics Express | 2013
Jacob Ramsay; Sune Dupont; Mikkel Johansen; Lars Søgaard Rishøj; Karsten Rottwitt; Peter M. Moselund; S. R. Keiding
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.
Journal of The Optical Society of America B-optical Physics | 2011
Christian Petersen; Sune Dupont; Christian Agger; Jan Thøgersen; Ole Bang; S. R. Keiding
We have measured the absolute Raman gain spectrum in short fluoride soft glass fibers with a pump wavelength of 1650 nm. We found a peak gain of gR=4.0±2×10−14 m W−1.
Laser Physics Letters | 2014
Sune Dupont; Z. Qu; Ssegawa-Ssekintu Kiwanuka; L. E. Hooper; Jonathan C. Knight; S. R. Keiding; Clemens F. Kaminski
We report the use of a dispersed supercontinuum generated in an all-normal-dispersion fibre to record low-noise spectra from atmospheric molecules at least an order of magnitude faster than has been previously reported. Supercontinuum generation in standard, anomalous dispersion photonic-crystal fibres is inherently connected with large pulse-to-pulse fluctuations resulting in detrimental consequences for high resolution spectroscopy if temporal averaging is not permitted. Replacing the standard photonic-crystal fibre (PCF) with a specially designed all-normal dispersion PCF we find that a substantially superior noise performance is achieved and present its use for high repetition rate absorption spectroscopy where spectra covering hundreds of nm in spectral bandwidth can be captured of gases at hundreds of kHz repetition rates.
Journal of The Optical Society of America B-optical Physics | 2013
Sune Dupont; Peter M. Moselund; Lasse Leick; Jacob Ramsay; S. R. Keiding
We present an cross-correlation frequency-resolved optical gating (XFROG) measurement of a megahertz IR supercontinuum generated in a step-index ZBLAN fiber. The resulting spectrogram gives the dispersion characteristics of the fiber and reveals that it has three zero-dispersion wavelengths. A comparison of the measured spectrogram with numerical simulations shows that this dispersion profile allows a notable dispersive-wave generation toward long wavelengths. Furthermore, the sum-frequency generation process in the XFROG measurement gives the possibility of measuring the IR light with fast Si-based detectors, such as CCD arrays.
Laser Physics Letters | 2014
Jacob Ramsay; Sune Dupont; S. R. Keiding
Infrared supercontinuum sources suffer from amplitude and polarization fluctuations. These fluctuations are seeded by stochastic noise, and thus limits the applicability of such sources. Here it is shown that implementation of polarization insensitive pulse-to-pulse normalization enhances the signal-to-noise ratio up to 18 times compared to conventional 45° beam splitting. This serves as a promising approach to achieve highly sensitive supercontinuum spectroscopy.
Applied Spectroscopy | 2016
Tine Ringsted; Sune Dupont; Jacob Ramsay; Birthe Møller Jespersen; Klavs Martin Sørensen; S. R. Keiding; Søren Balling Engelsen
The supercontinuum laser is a new type of light source, which combines the collimation and intensity of a laser with the broad spectral region of a lamp. Using such a source therefore makes it possible to focus the light onto small sample areas without losing intensity and thus facilitate either rapid or high-intensity measurements. Single seed transmission analysis in the long wavelength (LW) near-infrared (NIR) region is one area that might benefit from a brighter light source such as the supercontinuum laser. This study is aimed at building an experimental spectrometer consisting of a supercontinuum laser source and a dispersive monochromator in order to investigate its capability to measure the barley endosperm using transmission experiments in the LW NIR region. So far, barley and wheat seeds have only been studied using NIR transmission in the short wavelength region up to 1100 nm. However, the region in the range of 2260–2380 nm has previously shown to be particularly useful in differentiating barley phenotypes using NIR spectroscopy in reflectance mode. In the present study, 350 seeds (consisting of 70 seeds from each of five barley genotypes) in 1 mm slices were measured by NIR transmission in the range of 2235–2381 nm and oils from the same five barley genotypes were measured in a cuvette with a 1 mm path length in the range of 2003–2497 nm. The spectra of the barley seeds could be classified according to genotypes by principal component analysis; and spectral covariances with reference analysis of moisture, β-glucan, starch, protein and lipid were established. The spectral variations of the barley oils were compared to the fatty acid compositions as measured using gas chromotography–mass spectrometry (GC-MS).
conference on lasers and electro optics | 2015
Christian Rosenberg Petersen; Uffe Meller; Irnis Kubat; Binbin Zhou; Sune Dupont; Jacob Ramsay; Trevor M. Benson; S. Sujecki; Nabil Abdel-Moneim; Zhuoqi Tang; David Furniss; Angela B. Seddon; Ole Bang
Supercontinuum generation covering an ultra-broad spectrum from 1.5-11.7μm and 1.4-13.3μm is experimentally demonstrated by pumping an 85mm chalcogenide step-index fiber with 100fs pulses at a wavelength of 4.5μm and 6.3μm, respectively.