Abstract
Conventional lead isotope ratio measurements by thermal ionization mass spectrometry (TIMS) are currently limited to external precisions of ∼0.1% (2 σ) due to variations in instrumental mass discrimination, the magnitude of which can only be assessed using external standard or duplicate measurements. The goal of the double-spike technique, by contrast, is to circumvent this fractionation problem entirely by determining the mass discrimination factor ϵ directly for each sample. The unknown factor can be obtained after performing a second measurement on a sample aliquot to which a double spike of known, calibrated composition has been added. Practical applications of the double-spike technique up until now have used a mixed 207 Pb– 204 Pb tracer with considerable success, but there appears to have been little or no attempt to optimize the composition of the tracer used. An optimal tracer composition must fulfil two criteria: (1) the ratio of the internal, measured errors to a posteriori errors—the error magnification factors—should be as small as possible; (2) the propagated errors should not be strongly influenced by the spike/sample ratio of the second, mixture run—the latter is important since sample size cannot, in general, be rigorously controlled in advance. Of equal importance to the tracer composition itself is the choice of the three mass-balance equation set used to solve for ϵ; geometrically, this is equivalent to defining a mixing line in a particular 3D isotope space. Potential spike compositions were examined in four such 3D isotope spaces, corresponding to cases where 208 Pb, 207 Pb, 206 Pb and 204 Pb in turn are common, denominator isotopes of the ratios on the three orthogonal axes. Within each isotope space there exist three possible double-spike families. Tracers composed of three stable isotopes of lead—so-called `triple spikes'—are also considered, of which there are three families per isotope space. These spike compositions were evaluated for a typical common lead composition, at first using geometric methods, and then refined by determining error magnification factors using an ion statistical error model. It is shown that the 207 Pb– 204 Pb double spike used in previous studies, where ϵ is determined in 208,207,206 Pb/ 204 Pb isotope space, is one of the least suitable to use. Optimal tracer compositions for determining ϵ appear to be restricted to two families: The first is a family of 207 Pb– 204 Pb– 206 Pb triple spikes with 207 Pb/ 204 Pb of around unity and the isotope space has 206 Pb as the denominator isotope; the second family consists of 204 Pb– 207 Pb double spikes, solved in 208,206,204 Pb/ 207 Pb isotope space. Both of these families yield error magnification factors on a posteriori, corrected 206 Pb/ 204 Pb ratios as low as ∼1.2, and are less than 2 for all but highly underspiked and overspiked mixture compositions.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
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.