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Improved fluorescence peak integration in the Tekran 2537 for applications with sub-optimal sample loadings
Authors:PC Swartzendruber  DA Jaffe  B Finley
Institution:1. Department of Materials Engineering, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo 113-8656, Japan;2. NIMS Beamline Station at SPring-8, National Institute for Materials Science, Kouto 1-1-1, Sayo-cho, Sayo-gun, Hyogo 679-5198, Japan;3. International Center for Materials Nanoarchitectonics, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan;1. Taihu Laboratory for Lake Ecosystem Research, State Key Laboratory of Lake Science and Environment, Nanjing Institute of Geography and Limnology, Chinese Academy of Sciences, Nanjing 210008, China;2. University of Chinese Academy of Sciences, Beijing 100049, China;3. Sino-Danish Centre for Education and Research, Beijing 100190, China;4. Department of Bioscience and Arctic Research Centre, Aarhus University, Vejlsøvej 25, DK-8600 Silkeborg, Denmark;5. Yunnan Key Laboratory of Pollution Process and Management of Plateau Lake-Watershed, Yunnan Institute of Environmental Science, Kunming 650034, China
Abstract:The Tekran 2537 is widely used for monitoring atmospheric mercury. Although the instrument was designed for sample volumes in excess of 7.5 L, some recent research applications (e.g. aircraft) have used the instrument with significantly smaller collection times and sample volumes – and therefore smaller Hg loadings per cycle – than for which the instrument was designed. We have noticed a potential for non-linear (low) response in the fluorescence peak integration scheme, and thus the reported concentrations when the Hg loading (per cycle) is less than about 10–15 pg, e.g. at around 1 pg loading, the sensitivity is 25% lower than at 10 pg. We determined that although the atomic fluorescence detector was fundamentally linear down to at least 1 pg, the default peak integration scheme appeared to be optimized for > 10–15 pg cycle?1 and so could introduce non-linearity in smaller peaks (i.e. lower mass loadings). For research applications where achieving maximum accuracy and precision of individual, high-time resolution (<5 min) points is crucial, users can mitigate this behavior by modifying the integration parameters or recording the full fluorescence peak and processing the data offline. Two offline methods of quantifying the peak also improved the precision and thus suggest an improvement in the detection limit is possible.
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