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Discussion of shot noise limit with decreasing beam intensity: Shot noise was nicely defined by Merritt & Haye [1] and the shot noise limit (ï³ï¤), or the smallest standard error that can be reached based on counting statistics, can be calculated with the following equation: ï³ï¤2 = 2 x 106 * (ï³R/R)2 (S1) This can be rewritten as: ï³ï¤2 = 2 x 106 * (1+R)/R * (ï44*qe)/(t*V44) (S2) Figure S15: Mass of reacted carbonate vs calculated (line) and observed (points) shot noise limit. 0.005 shot noise limit (permil) 0.010 0.015 0.020 where R is the ratio of the number of ions collected per time unit (current) in the mass of interest (47) relative to the most common mass (44) (=i47/i44 = 4.8x10-5), ï44 is the resistor on m/z 44 (=3x107 ohms), and qe is the charge on each ion (=1.6x10-19 C). In the traditional dual-bellows measurement configuration, V44 is the target voltage for the m/z 44 beam at which every cycle is measured. The quantity V44*t/qe, where t is the total number of seconds of integration time over all cycles and acquisitions, gives an estimate of the total number of ions collected over the whole measurement period. In our dual-reservoir measurement configuration, the beam intensity (and therefore V44) is constantly changing throughout the run. In order to quantify the total number of ions collected over the measurement period, we âintegrateâ the beam strength over time. We take V44 for each cycle, multiply by 26 seconds, the integration time of a single cycle, and then sum all the cycles. This is computationally equivalent to taking the average V44 value over the whole run and inputting that in place of the target voltage V44 in the equation above. We observe a linear relationship between the average V44 and the initial V47, which we can relate to sample size by the following equations: V44-average = 0.4197* V47-initial + 50.2 V47-initial = 2231*(Mass of CaCO3) -1714 These equations are defined based on the sensitivity levels observed during this study (Smaller U-trap, tuning 2), and would change with changes in sensitivity. We can use Sample Size vs. Shot noise limit (for 7acquisitions x 14 cycles) these equations to plot the shot noise limit against sample size, assuming that all samples were run Calculated from equations for the same amount of time (7 Measured 1sigma SE on D47 acquisitions x 14 cycles x 26 second integration time). We see our measured standard error increasing in line with the predicted shot noise limit at small sample sizes. 1.0 17 1.5 2.0 mass of reacted carbonate (mg) 2.5