Fig. 7
Same as Fig. 3, but for 20 u q−1. Stacked spectra in low resolution (top panel) and in HR at 20 u q−1 (bottom). The HR spectra at 20 u q−1 are already shown in Fig. 6. As one may see, the DFMS mass-per-charge resolution cannot separate: H3 17O+ from H2DO+. In addition, the peak in LR at 19 u q−1 is at the edge of the detector such that it is only partially resolved.
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