Bring a δ value measured against one standard onto the scale of another, using the published offsets between the two: the page gives the converted value, its propagated uncertainty and the source of each offset. When no published calibration links two standards, it says so and computes nothing.
Choose the system, your isotope ratio and the two standards. Each measured lot or bottle is a separate entry: pick the one you use.
The name of a standard says nothing about its composition. Two bottles of SPEX PLSN5 tin solution carrying the same lot number were measured 0.26 ‰ apart in δ122/118Sn, while lots of the same maker's CLSN2 range are identical to each other (Meister et al., 2026).
The page therefore links two standards only through measured and published offsets, each referred to the scale zero of its system. Without a published offset, it gives no value.
a and b are the values of standards A and B on the common scale. This is the composition of isotope ratios, set out by Meister et al. (2026, equation 6). The usual additive form δA + a − b departs from it by about δ·a/1000: negligible for offsets of a few tenths of a per mil, noticeable for offsets of several per mil, as between V-PDB and V-SMOW.
Each uncertainty is brought to one standard deviation: a published 2SD or 2SE is halved, an expanded uncertainty divided by its coverage factor k. It is weighted by the derivative of the exact formula, then returned in your convention.
The two offsets are treated as independent; when they come from the same study, the uncertainty is probably overestimated. A reproducibility 2SD is read as two standard deviations, the usual reading, which remains narrower than a full calibration uncertainty.
If you measure another ratio than the calibrations, 122Sn/118Sn instead of 124Sn/116Sn for instance, the offsets between standards are carried over with the mass-dependent fractionation law (Wombacher and Rehkämper, 2004), exponential or equilibrium. Only those offsets are transformed, never your value: a mass-independent anomaly it may carry, such as Δ199Hg or Δ33S, stays intact. The page shows what the other law would give.
References: Meister, A.C.E. et al. (2026). A Common Reference Material for Mass-Dependent Sn Isotope Compositions: An Inter-Laboratory Calibration Approach. Geostandards and Geoanalytical Research, 50(2), 341-367. doi:10.1111/ggr.70035. Wombacher, F. and Rehkämper, M. (2004). Problems and Suggestions Concerning the Notation of Cadmium Stable Isotope Compositions and the Use of Reference Materials. Geostandards and Geoanalytical Research, 28(1), 173-178. doi:10.1111/j.1751-908x.2004.tb01054.x.
Each standard with its value on the scale of its system's zero, the uncertainty as published and the source. Notes on each standard are in French.
These systems and standards appear in Atlas records, but no published offset links them to another standard in the database: the page offers no conversion for them. Radiogenic ratios (lead, strontium, neodymium, osmium) call for a different approach, renormalisation to the reference value of the standard.
Please also cite the publication behind each offset you use: the result copied from the converter lists the references.
Converting a single value is free. Inside the Atlas, the sample comparison brings published ranges to your standard by itself, and Atlas access adds batch conversion, notation changes and export.
IsoFind brings together several services around isotope geochemistry. The Atlas gathers published values for ore deposits, contaminated sites and fractionation, free to browse, with more than 1,300 reference pages in English and French. The IsoFind software is for working on your own measurements, offline. Free online tools such as the standards conversion and two open formats, ISOF and IGL, complete it. Each page of the site shows only part of this whole: the links below lead to the rest.
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