Abstract

Abstract. Over the last few decades, differential optical absorption spectroscopy (DOAS) has been used as a common technique to simultaneously measure abundances of a variety of atmospheric trace gases. Exploiting the unique differential absorption cross section of trace-gas molecules, mixing ratios can be derived by measuring the optical density along a defined light path and by applying the Beer–Lambert law. Active long-path (LP-DOAS) instruments can detect trace gases along a light path of a few hundred metres up to 20 km, with sensitivities for mixing ratios down to ppbv and pptv levels, depending on the trace-gas species. To achieve high measurement accuracy and low detection limits, it is crucial to reduce instrumental artefacts that lead to systematic structures in the residual spectra of the analysis. Spectral residual structures can be introduced by most components of a LP-DOAS measurement system, namely by the light source, in the transmission of the measurement signal between the system components or at the level of spectrometer and detector. This article focuses on recent improvements by the first application of a new type of light source and consequent changes to the optical setup to improve measurement accuracy. Most state-of-the-art LP-DOAS instruments are based on fibre optics and use xenon arc lamps or light-emitting diodes (LEDs) as light sources. Here we present the application of a laser-driven light source (LDLS), which significantly improves the measurement quality compared to conventional light sources. In addition, the lifetime of LDLS is about an order of magnitude higher than of typical Xe arc lamps. The small and very stable plasma discharge spot of the LDLS allows the application of a modified fibre configuration. This enables a better light coupling with higher light throughput, higher transmission homogeneity, and a better suppression of light from disturbing wavelength regions. Furthermore, the mode-mixing properties of the optical fibre are enhanced by an improved mechanical treatment. The combined effects lead to spectral residual structures in the range of 5-10×10-5 root mean square (rms; in units of optical density). This represents a reduction of detection limits of typical trace-gas species by a factor of 3–4 compared to previous setups. High temporal stability and reduced operational complexity of this new setup allow the operation of low-maintenance, automated LP-DOAS systems, as demonstrated here by more than 2 years of continuous observations in Antarctica.

Highlights

  • Active long-path differential optical absorption spectroscopy (LP-DOAS) is a well-established remote-sensing technique based on the DOAS principle introduced by Perner et al (1976) and Platt and Perner (1980, 1983)

  • The crucial components in a modern fibre-based LP-DOAS setup are the light source and a Y-shaped optical fibre bundle, where one end serves as sending fibre bundle that guides the light from the light source to the telescope and the other end serves as a receiving fibre bundle, leading from the telescope to the spectrometer

  • We present a series of improvements to fibre-based long-path differential optical absorption spectroscopy (LPDOAS) systems and discuss their respective contributions to the overall improvement of the measurement accuracy and precision

Read more

Summary

Introduction

Active long-path differential optical absorption spectroscopy (LP-DOAS) is a well-established remote-sensing technique based on the DOAS principle introduced by Perner et al (1976) and Platt and Perner (1980, 1983). It can attain detection limits on the order of ppbv to pptv (nanomole per mole to picomole per mole) for absorbers in the ultraviolet to near-infrared spectral range (270–800 nm). Improvements of measurement performance and operation procedure following the introduction of the novel light source and changes to the fibre configuration are presented in Sect.

Long-path DOAS
State-of-the-art instrument setup
DOAS analysis and measurement accuracy
LP-DOAS setups used in this study
Light sources and fibre configurations
Comparison of light sources
Adaptation of the optical setup to the light source
Fibre bundle configurations
Comparison of instrumental stray light
Fibre modes
Method
Temporal stability of mode-mixing methods
The optimal mode-mixing setup
Intercomparison measurements in Heidelberg
Conclusions
Findings
Bandpass filters used in stray-light investigation

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.