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dc.contributor.authorBernhardt, B
dc.contributor.authorSorokin, E
dc.contributor.authorJacquet, P
dc.contributor.authorThon, R
dc.contributor.authorBecker, T
dc.contributor.authorSorokina, Irina T
dc.contributor.authorPicque, N
dc.contributor.authorHansch, TW
dc.date.accessioned2017-11-02T07:55:46Z
dc.date.available2017-11-02T07:55:46Z
dc.date.created2010-11-02T13:16:26Z
dc.date.issued2010
dc.identifier.citationApplied physics B. 2010, 100 (1), 3-8.nb_NO
dc.identifier.issn0946-2171
dc.identifier.urihttp://hdl.handle.net/11250/2463578
dc.description.abstractThe mid-infrared part of the electromagnetic spectrum is the so-called molecular fingerprint region because gases have tell-tale absorption features associated with molecular rovibrations. This region can be for instance exploited to detect small traces of environmental and toxic vapors in atmospheric and industrial applications. Novel Fourier-transform spectroscopy without moving parts, based on time-domain interferences between two comb sources, can in particular benefit optical diagnostics and precision spectroscopy. To date, high-resolution and -sensitivity proof-of-principle experiments have only been reported in the near-infrared region where frequency-comb oscillators are conveniently available. However, as most of the molecular transitions in this region are due to weak overtone bands, this spectral domain is not ideal for sensitive and rapid detection. Here we present a proof-of-principle experiment of frequency-comb Fourier-transform spectroscopy with two Cr2+:ZnSe femtosecond oscillators directly emitting in the 2.4 μm mid-infrared region. The acetylene absorption spectrum in the region of the n1+n511+51 band, extending from 2370 to 2525 nm, could be recorded within a 10 μs acquisition time without averaging with 12 GHz resolution.nb_NO
dc.language.isoengnb_NO
dc.titleMid-infrared dual-comb spectroscopy with 2.4 mu m Cr2+:ZnSe femtosecond lasersnb_NO
dc.typeJournal articlenb_NO
dc.description.versionsubmittedVersionnb_NO
dc.source.pagenumber3-8nb_NO
dc.source.volume100nb_NO
dc.source.journalApplied physics Bnb_NO
dc.source.issue1nb_NO
dc.identifier.doi10.1007/s00340-010-4080-0
dc.identifier.cristin349545
dc.description.localcode© Springer Verlag. The final publication is available at https://link.springer.com/article/10.1007%2Fs00340-010-4080-0. This is the authors' manuscript to the article.nb_NO
cristin.unitcode194,66,20,0
cristin.unitnameInstitutt for fysikk
cristin.ispublishedtrue
cristin.fulltextpreprint
cristin.qualitycode1


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