M. Gianella, Akshay Nataraj, B. Tuzson, F. Kapsalidis, S. Schilt, T. Südmeyer, J. Faist, L. Emmenegger
{"title":"Spectral Interleaving with Quantum Cascade Laser Frequency Combs","authors":"M. Gianella, Akshay Nataraj, B. Tuzson, F. Kapsalidis, S. Schilt, T. Südmeyer, J. Faist, L. Emmenegger","doi":"10.1109/CLEOE-EQEC.2019.8873290","DOIUrl":null,"url":null,"abstract":"Quantum cascade laser (QCL) based frequency combs are mid-infrared sources capable of producing hundreds of mW of optical power distributed across several hundred comb lines spanning tens of cm−1. In the dual comb (or multi-heterodyne) configuration, two nearly identical frequency combs with slightly different comb spacing are used as an interrogating and local oscillator comb, respectively, to probe the absorption or refractive index of a sample [1]. The multi-heterodyne beat note signal produced by overlapping the two beams on a fast photodetector allows simultaneous access to all optical frequencies of the interrogating comb, enabling fast (sub-μs) acquisition of time-resolved absorption and/or dispersion spectra [2]. The typical length of QCL devices of ca. 5 mm leads to comb spacings of the order of 10 GHz (0.33 cm−1). While suitable for spectroscopy in the condensed phase, gas-phase spectroscopy requires much finer spectral sampling (e.g. <10 MHz for Doppler-broadened transitions of small molecules). This can be achieved by spectral interleaving, i.e. by the continuous or step-wise shifting of the spectrum of the interrogating comb.","PeriodicalId":6714,"journal":{"name":"2019 Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC)","volume":"30 1","pages":"1-1"},"PeriodicalIF":0.0000,"publicationDate":"2019-10-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2019 Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CLEOE-EQEC.2019.8873290","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Quantum cascade laser (QCL) based frequency combs are mid-infrared sources capable of producing hundreds of mW of optical power distributed across several hundred comb lines spanning tens of cm−1. In the dual comb (or multi-heterodyne) configuration, two nearly identical frequency combs with slightly different comb spacing are used as an interrogating and local oscillator comb, respectively, to probe the absorption or refractive index of a sample [1]. The multi-heterodyne beat note signal produced by overlapping the two beams on a fast photodetector allows simultaneous access to all optical frequencies of the interrogating comb, enabling fast (sub-μs) acquisition of time-resolved absorption and/or dispersion spectra [2]. The typical length of QCL devices of ca. 5 mm leads to comb spacings of the order of 10 GHz (0.33 cm−1). While suitable for spectroscopy in the condensed phase, gas-phase spectroscopy requires much finer spectral sampling (e.g. <10 MHz for Doppler-broadened transitions of small molecules). This can be achieved by spectral interleaving, i.e. by the continuous or step-wise shifting of the spectrum of the interrogating comb.