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. Author manuscript; available in PMC: 2020 Mar 12.
Published in final edited form as: J Radioanal Nucl Chem. 2019;322(3):10.1007/s10967-019-06711-6. doi: 10.1007/s10967-019-06711-6

Table 4.

IDMS sample data and measurement results for the molality of 231Pa in the RM solution

Sample ID 231Pa RM solution aliquots (g) 233Pa spike aliquots (g) Measured isotope ratio* n(233Pa)/n(231Pa) Molality of 231Pa (pmol g−1)
231Pa 1 0.6318 ± 0.0010 3.0843 ± 0.0010 0.016894 ± 0.000046 27.56 ± 0.13
231Pa 2 1.0531 ± 0.0010 3.5580 ± 0.0010 0.011701 ± 0.000048 27.54 ± 0.11
231Pa 3 0.7848 ± 0.0010 3.4152 ± 0.0010 0.015067 ± 0.000047 27.55 ± 0.14
231Pa 4 0.5688 ± 0.0010 3.4580 ± 0.0010 0.021023 ± 0.000044 27.58 ± 0.12
231Pa 5 0.8931 ± 0.0010 3.1462 ± 0.0010 0.012203 ± 0.000055 27.53 ± 0.16

For IDMS calculations, the molality of 233Pa in the S solution was decay corrected to the time of final purification for the protactinium IDMS mixes, 14 July 2017 18:20 UTC. Uncertainties are expanded uncertainties (U=kuc) with a coverage factor (k) of 2. All mass values are corrected for air buoyancy

*

A correction factor (0.99936 ± 0.00059) was applied to measured n(233Pa)/n(231Pa) ratios to account for mass spectrometer efficiency differences between 233Pa and 233U. The correction factor was calculated based on the relative proportion of 233U that grew in over the interval between purification and the mass spectrometer measurements and an observed transmission efficiency difference between uranium and protactinium (8.7%). This transmission difference was empirically determined based on the bias between the measured n(233Pa)/n(231Pa) ratio of a mixed solution and the n(233U)/n(231Pa) ratio of the same solution after the decay of 233Pa