In 2015 Barkan et al performed high‐precision measurements of the δ17O and 17Oexcess values of the international carbonate standards NBS19 and NBS18.1 In 2016 a new standard (IAEA‐603) was introduced, aimed to replace NBS19 that had been exhausted, as the new international standard for δ13C and δ18O analyses.2 In order to use it also as a standard for 17Oexcess, we present here high‐precision measurements of three oxygen isotopes in this standard.
The measurements were carried out by direct oxygen isotope exchange between CO2 extracted from CaCO3 and O2 of known three oxygen isotopic composition, followed by analysis of the resulting O2 for δ17O and δ18O values. These values were used to calculate 17Oexcess as:
17Oexcess = 106 [ln(10−3δ17O + 1) − 0.528 ln(10−3δ18O + 1)].
All methodological details, including those for CO2 extraction from carbonates, were given previously.1 In short, CO2 samples were extracted from CaCO3 by digestion with 1.92 g/cm3 phosphoric acid at 25°C. The CO2 underwent isotopic exchange with O2 of a known isotopic composition over hot platinum. After isotope exchange, the O2 samples were measured by dual‐inlet mass spectrometry versus an O2 working reference gas that was calibrated with respect to VSMOW. The obtained values were then normalized to the VSMOW–SLAP scale, assuming that the 17Oexcess value of SLAP equals zero.3 As the 17O isotopic fractionation for phosphoric acid digestion is unknown, the reported values are for the CO2 rather than for CaCO3.4
All measurements were performed alongside an in‐house CO2 standard that was analyzed daily to check the performance of the CO2‐O2 isotope exchange setup and of the mass spectrometer. This standard was accurately calibrated for 17Oexcess using CO2 equilibrated with waters of different three oxygen isotopic compositions, as well as CO2 produced by quantitative conversion over hot graphite of pre‐calibrated O2 gas to CO2 with a known three oxygen isotopic composition.5, 6 On days in which the measured 17Oexcess value of this in‐house CO2 standard was offset from the long‐term mean, a correction was applied to the values obtained for all samples measured on that day.
Two different ampoules of IAEA‐603 were analyzed for their δ17O and 17Oexcess values. In order to minimize the effect of potential unrecognized analytical errors, replicate analyses were performed on different days and the full set of measurements was repeated 6 months apart. Each CO2 sample was measured for its δ18O value versus a working reference gas that was previously calibrated using NBS19. The average δ18O value of IAEA‐603 was −2.35 ± 0.03‰ versus VPDB, which is within analytical error from the IAEA certified value (−2.37± 0.04‰).2 The small difference of 0.02‰ introduces only a negligible error in the calculation of CO2 17Oexcess values, and thus we normalized our δ18O data to the nominal value.
Data of 17Oexcess are given in Table 1. As can be seen, 17Oexcess values varied by 5–6 per meg among replicates, and the two ampoules differed by only 3 per meg, less than our analytical error. This suggests that this standard is homogenous with respect to 17Oexcess. The resulting mean value of 17Oexcess of CO2 extracted from IAEA‐603 at 25°C is −194 ± 6 per meg.
Table 1.
δ17O, δ18O and 17Oexcess values of CO2 extracted from IAEA‐603 at 25°C. All values are versus VSMOW; δ17O and δ18O in ‰, 17Oexcess in per meg. Errors of the mean correspond to the 95% confidence limit (standard error of the mean multiplied by Student's t‐factor)
Date | δ17O | δ18Oa | 17Oexcess |
---|---|---|---|
Ampoule 1 | |||
19/12/17 | 20.214 | 39.019 | −198 |
25/12/17 | 20.211 | 39.019 | −201 |
26/12/17 | 20.217 | 39.019 | −195 |
02/01/18 | 20.228 | 39.019 | −184 |
03/01/18 | 20.221 | 39.019 | −191 |
07/01/18 | 20.212 | 39.019 | −200 |
13/05/18 | 20.223 | 39.019 | −189 |
15/05/18 | 20.213 | 39.019 | −199 |
16/06/18 | 20.214 | 39.019 | −198 |
27/06/18 | 20.215 | 39.019 | −197 |
01/07/18 | 20.216 | 39.019 | −196 |
Aver. | 20.217 | 39.019 | −195 |
± SE*t | 0.005 | 5 | |
Ampoule 2 | |||
27/12/17 | 20.221 | 39.019 | −191 |
28/12/17 | 20.212 | 39.019 | −200 |
24/01/18 | 20.227 | 39.019 | −185 |
25/01/18 | 20.222 | 39.019 | −190 |
29/01/18 | 20.228 | 39.019 | −184 |
15/05/18 | 20.222 | 39.019 | −190 |
16/05/18 | 20.215 | 39.019 | −197 |
25/06/18 | 20.221 | 39.019 | −191 |
26/06/18 | 20.212 | 39.019 | −200 |
01/07/18 | 20.224 | 39.019 | −188 |
02/07/18 | 20.215 | 39.019 | −197 |
Aver. | 20.220 | 39.019 | −192 |
± SE*t | 0.006 | 6 | |
Grand averages | δ17O = 20.218 ± 0.005; δ18O = 39.019; 17Oexcess = − 194 ± 6 |
Whereas 17Oexcess values of NBS19 and NBS18 have been previously measured at high precision, there is a clear discrepancy between the values measured in our laboratory1 and those measured by Passey et al.8 Therefore, we re‐measured the 17Oexcess values of NBS19 and NBS18 alongside the measurements of IAEA‐603 to verify the exact relationship between the three standards. Unfortunately, the materials in the bottles of NBS19 and NBS18 used in 2015 were exhausted and, hence, the exact same materials could not be re‐measured. Accordingly, measurements were performed using a new bottle (purchased in 2016) for each of the two standards.
Our CO2 working reference gas has been calibrated for δ18O using NBS19. Therefore, our average δ18O value of NBS19 is the same as the IAEA certified value,7 within our analytical precision (0.03‰). The measured δ18O value for NBS18 was slightly higher than the nominal value7 (offset by 0.07‰), although it is still within the uncertainty estimate given by the IAEA for this standard (0.22‰). As noted above, such small differences in δ18O values introduce only a negligible error in the calculated CO2 17Oexcess values, and thus we used the IAEA nominal values in our calculations.
The obtained 17Oexcess values were −178 ± 4 per meg for NBS19 and −162 ± 5 per meg for NBS18 (Bottle 1 in Tables 2 and 3). These results are surprising as both values differ significantly from those that we measured a few years ago1 −227 per meg for NBS19 and 3 per meg for NBS18. At the same time, our in‐house Carrara marble, which has been systematically measured over these 3 years, shows stable 17Oexcess values within the analytical precision.
Table 2.
δ17O, δ18O and 17Oexcess values of CO2 extracted from NBS19 at 25°C. All values are versus VSMOW; δ17O and δ18O in ‰, 17Oexcess in per meg. Errors of the mean correspond to the 95% confidence limit (standard error of the mean multiplied by Student's t‐factor)
Sample | Date | δ17O | δ18Oa | 17Oexcess |
---|---|---|---|---|
Bottle 1 (IAEA) | 27/12/17 | 20.320 | 39.196 | −184 |
28/12/17 | 20.331 | 39.196 | −173 | |
03/01/18 | 20.323 | 39.196 | −181 | |
04/01/18 | 20.323 | 39.196 | −181 | |
07/01/18 | 20.330 | 39.196 | −174 | |
07/01/18 | 20.321 | 39.196 | −183 | |
24/01/18 | 20.330 | 39.196 | −174 | |
25/01/18 | 20.325 | 39.196 | −179 | |
26/01/18 | 20.329 | 39.196 | −175 | |
28/01/18 | 20.331 | 39.196 | −173 | |
31/01/18 | 20.325 | 39.196 | −179 | |
03/05/18 | 20.332 | 39.196 | −172 | |
03/05/18 | 20.321 | 39.196 | −178 | |
06/05/18 | 20.324 | 39.196 | −175 | |
07/06/18 | 20.319 | 39.196 | −180 | |
08/06/18 | 20.323 | 39.196 | −181 | |
09/06/18 | 20.325 | 39.196 | −179 | |
Aver. | 20.325 | 39.196 | −178 | |
± SE*t | 0.004 | 4 | ||
Bottle 2 (IAEA) | 07/05/18 | 20.325 | 39.196 | −179 |
08/05/18 | 20.326 | 39.196 | −178 | |
10/05/18 | 20.326 | 39.196 | −178 | |
24/05/18 | 20.316 | 39.196 | −188 | |
25/05/18 | 20.325 | 39.196 | −179 | |
27/05/18 | 20.321 | 39.196 | −183 | |
27/05/18 | 20.319 | 39.196 | −185 | |
Aver. | 20.323 | 39.196 | −181 | |
± SE*t | 0.004 | 4 | ||
Bottle 3 (IAEA) | 12/05/18 | 20.316 | 39.196 | −188 |
13/05/18 | 20.317 | 39.196 | −187 | |
21/05/18 | 20.311 | 39.196 | −193 | |
24/06/18 | 20.317 | 39.196 | −187 | |
25/06/18 | 20.317 | 39.196 | −186 | |
27/06/18 | 20.315 | 39.196 | −189 | |
Aver. | 20.315 | 39.196 | −188 | |
± SE*t | 0.003 | 3 | ||
Bottle 4 (NIST) | 09/05/18 | 20.312 | 39.196 | −192 |
14/05/18 | 20.318 | 39.196 | −186 | |
16/05/18 | 20.312 | 39.196 | −192 | |
12/06/18 | 20.307 | 39.196 | −197 | |
14/06/18 | 20.317 | 39.196 | −187 | |
16/06/18 | 20.320 | 39.196 | −184 | |
21/06/18 | 20.326 | 39.196 | −178 | |
27/06/18 | 20.323 | 39.196 | −181 | |
28/06/18 | 20.315 | 39.196 | −189 | |
Aver. | 20.317 | 39.196 | −187 | |
± SE*t | 0.006 | 6 | ||
Grand averages | δ17O = 20.320 ± 0.006; δ18O = 39.196; 17Oexcess = −182 ± 6 |
Table 3.
δ17O, δ18O and 17Oexcess values of CO2 extracted from NBS18 at 25°C. All values are versus VSMOW; δ17O and δ18O in ‰, 17Oexcess in per meg. Errors of the mean correspond to the 95% confidence limit (standard error of the mean multiplied by Student's t‐factor)
Sample | Date | δ17O | δ18Oa | 17Oexcess |
---|---|---|---|---|
Bottle 1 (IAEA) | 02/01/18 | 9.057 | 17.522 | −155 |
03/01/18 | 9.048 | 17.522 | −164 | |
04/01/18 | 9.043 | 17.522 | −169 | |
04/01/18 | 9.054 | 17.522 | −158 | |
07/01/18 | 9.050 | 17.522 | −162 | |
29/01/18 | 9.052 | 17.522 | −160 | |
03/05/18 | 9.056 | 17.522 | −156 | |
06/05/18 | 9.045 | 17.522 | −167 | |
07/05/18 | 9.056 | 17.522 | −156 | |
08/05/18 | 9.046 | 17.522 | −166 | |
02/06/18 | 9.047 | 17.522 | −165 | |
03/06/18 | 9.049 | 17.522 | −163 | |
04/06/18 | 9.046 | 17.522 | −166 | |
Aver. | 9.050 | 17.522 | −162 | |
± SE*t | 0.005 | 5 | ||
Bottle 2 (IAEA) | 12/05/18 | 9.049 | 17.522 | −163 |
13/05/18 | 9.045 | 17.522 | −167 | |
21/05/18 | 9.056 | 17.522 | −156 | |
24/06/18 | 9.054 | 17.522 | −159 | |
25/06/18 | 9.055 | 17.522 | −158 | |
26/06/18 | 9.043 | 17.522 | −169 | |
Aver. | 9.050 | 17.522 | −162 | |
± SE*t | 0.005 | 5 | ||
Bottle 3 (NIST) | 10/05/18 | 9.043 | 17.522 | −169 |
13/05/18 | 9.052 | 17.522 | −160 | |
14/05/18 | 9.042 | 17.522 | −170 | |
15/06/18 | 9.043 | 17.522 | −169 | |
16/06/18 | 9.042 | 17.522 | −171 | |
17/06/18 | 9.048 | 17.522 | −164 | |
Aver. | 9.045 | 17.522 | −167 | |
± SE*t | 0.004 | 4 | ||
Grand averages | δ17O = 9.049 ± 0.005; δ18O = 17.522; 17Oexcess = −163 ± 5 |
The simplest possible explanation for the difference between the two data sets is heterogeneity of 17Oexcess values among bottles of these standards. This may be due to inter‐bottle differences within a batch of standards, differences between old (older than ~30 years) and new batches of these materials, or variations between bottles prepared by IAEA and NIST. In addition, it is possible that the specific bottles that we used previously have been compromised over many years of use.
Because the specific materials analyzed previously are unavailable, it was impossible to test directly for heterogeneity between these old bottles and the current batch of standards. Instead, we measured 17Oexcess values in several different bottles of each standard. These bottles included materials prepared by both IAEA and NIST, with variable time of purchase. This allowed us to test for inter‐bottle heterogeneity and for potential differences between the two sources of standard materials. As can be seen in Tables 2 and 3, there are no significant differences between bottles, irrespective if the materials were prepared by IAEA or NIST. It is therefore most likely that the problem was specifically with the materials that we used in 2015 that may have been slightly contaminated, resulting in an δ17O offset.
It is important to note that in order to verify the accuracy of our values, in parallel to the carbonates analyses we measured CO2 that was equilibrated with different waters of known 17Oexcess values. The expected 17Oexcess values for these CO2 samples were calculated from the δ17O and δ18O values of the waters using CO2–H2O equilibrium fractionation factors.9 The waters were our in‐house water standards, which were well calibrated on the VSMOW–SLAP scale and cover a wide range of δ18O values (from −4‰ to −58‰ versus VSMOW). We also used water mixtures that were prepared such that the δ18O values of equilibrated CO2 would be similar to that of the CO2 extracted from NBS19 and NBS18. The agreement with the expected 17Oexcess values (within 5 per meg) in these CO2 samples5 serves to support the accuracy of our carbonate 17Oexcess values.
Farquhar et al10 measured a δ17O value in CO2 extracted from NBS18 by acid digestion followed by fluorination of the CO2 to release O2. The reported 17Oexcess value was calculated with respect to a reference slope of 0.52. The precision given for these data is too low to reliably convert the 17Oexcess value to a scale based on a different reference slope, and makes a direct comparison impractical. Liang et al11 reported a single measurement of CO2 extracted from NBS18 and analyzed by CO2–O2 exchange, as in our case, using the setup and protocol of Mahata et al.13 The resulting 17Oexcess value is 90 per meg relative to a reference slope of 0.516. Assuming the nominal IAEA δ18O value for NBS18 (17.522‰), we can estimate an 17Oexcess value of −119 per meg relative to a reference slope of 0.528. This value is between our value and that of Passey et al. Unfortunately, because Liang et al do not provide their measured δ18O and δ17O values, it is difficult to assess the accuracy of this value.
The first high‐precision measurements of 17Oexcess values in NBS18 and NBS19 were performed by Passey et al.8 Our new values are in much better agreement with their data (Table 4) relative to our 2015 values, although some differences remain. We note that the methods used in the two laboratories are very different. Whereas we report directly 17Oexcess in CO2 extracted from carbonates, Passey et al report 17Oexcess in O2 derived from water that, in turn, is produced by methanation of CO2. Furthermore, the extraction of CO2 from CaCO3 was performed by acid digestion under different conditions: 25°C in McCrea‐type vessels in our laboratory versus 90°C in a common acid bath in Passey et al. The fractionation in the acid digestion reaction is known for 18O, but not for 17O, and the 18α/17α ratio may be temperature dependent, resulting in different 17Oexcess values in the CO2 evolved in the two laboratories. As such, it should not be expected that the absolute 17Oexcess values agree. However, as the methodological differences are systematic, it is expected that the difference between two samples (namely, NBS19 and NBS18) would be consistent across methods. The observed discrepancy of 17 per meg between the two data sets (Table 4) is within the combined analytical precision (19 per meg). Furthermore, the consistency of measured and expected 17Oexcess values in CO2 equilibrated with isotopically known waters provides strong support for the robustness of our current values for CO2 extracted from CaCO3. We therefore suggest using the 17Oexcess values reported here in all three international standards for normalizing triple oxygen isotope data in carbonates, in order to enable meaningful comparisons of results among laboratories.
Table 4.
Comparison of the 17Oexcess values (per meg) of NBS19 and NBS18a
Present work | Passey et al8 | |
---|---|---|
NBS19 | −182 | −135 |
NBS18 | −163 | −98 |
Difference | 20 | 37 |
Note that the values in the present study were obtained by acid digestion of the carbonates at 25°C and are reported for CO2. In Passey et al8 CO2 was obtained by acid digestion at 90°C, and the values are reported for O2 produced by water fluorination, which in turn was obtained by methanation of extracted CO2.
As noted by Mahata et al,12 CO2 and O2 exchange over hot platinum is a heterogeneous reaction involving adsorption, desorption, and catalytic exchange. There may also be isotope effects associated with thermal diffusion between the cold and hot parts of the preparation lines. As a result, the empirical values of 17α and 18α are a combination of the fractionations in all the processes operating in the exchange reaction, and they therefore differ from the modeled values of equilibrium fractionations between CO2 and O2.12 These empirical values should be considered as effective, or apparent, steady‐state fractionations, rather than true equilibrium fractionation factors. Being empirical fractionation factors, they may vary among different experimental setups as well as depending on suppliers (or even batches) of the Pt sponge catalyst. Therefore, they may potentially vary over time and affect the resulting 17Oexcess values. These variations can be corrected for by routine measurements of in‐house standards, calibrated using IAEA‐603, NBS19 and NBS18.
ACKNOWLEDGEMENTS
We are grateful to Sergey Assonov for graciously providing ampoules of the new IAEA‐603 standard and for helpful discussions. Special thanks to our colleagues Faina Gelman, Ruth Yam, and Orit Sivan who shared their bottles of NBS19 and NBS18 standards. This research was supported by ERC (Grant SPADE‐724097) to HPA and ISF‐NSFC joint research program (Grant No. 633/15) to BL. We also thank two anonymous reviewers for valuable comments.
Barkan E, Affek HP, Luz B, Bergel SJ, Voarintsoa NRG, Musan I. Calibration of δ17O and 17Oexcess values of three international standards: IAEA‐603, NBS19 and NBS18. Rapid Commun Mass Spectrom. 2019;33:737–740. 10.1002/rcm.8391
REFERENCES
- 1. Barkan E, Musan I, Luz B. High‐precision measurements of δ17O and 17O‐excess of NBS‐19 and NBS‐18. Rapid Commun Mass Spectrom. 2015;29(23):2219‐2224. [DOI] [PubMed] [Google Scholar]
- 2. International Atomic Energy Agency , Reference Sheet for IAEA‐603. IAEA, Vienna, 2016‐08‐28, 7pp, https://nucleus.iaea.org/rpst/referenceproducts/referencematerials/Stable_Isotopes/13C18and7Li/IAEA‐603/RM603_Reference_Sheet_2016‐08‐16.pdf
- 3. Schoenemann SW, Schauer AJ, Steig EJ. Measurement of SLAP2 and GISP δ 17O and proposed VSMOW‐SLAP normalization δ 17O and 17Oexcess . Rapid Commun Mass Spectrom. 2013;27(5):582‐590. [DOI] [PubMed] [Google Scholar]
- 4. Brand WA, Assonov SS, Coplen TB. Correction for the 17O interference in δ 13C measurements when analyzing CO2 with stable isotope mass spectrometry (IUPAC technical report). Pure Appl Chem. 2010;82(8):1719‐1733. [Google Scholar]
- 5. Affek HP, Barkan E. A new method for high precision measurements of 17O/16O ratio in H2O. Rapid Commun Mass Spectrom. 2018;32(23):2096‐2097. [DOI] [PubMed] [Google Scholar]
- 6. Barkan E, Luz B. Conversion of O2 into CO2 for the high‐precision oxygen isotope measurements. Anal Chem. 1996;68(19):3507‐3510. [DOI] [PubMed] [Google Scholar]
- 7. Brand WA, Coplen TB, Vogl J, Rosner M, Prohaska T. Assessment of international reference materials for isotope‐ratio analysis (IUPAC technical report). Pure Appl Chem. 2014;86(3):425‐467. [Google Scholar]
- 8. Passey BH, Hu H, Ji H, et al. Triple oxygen isotopes in biogenic and sedimentary carbonates. Geochim Cosmochim Acta. 2014;141:1‐25. [Google Scholar]
- 9. Barkan E, Luz B. High‐precision measurements of 17O/16O and 18O/16O ratios in CO2 . Rapid Commun Mass Spectrom. 2012;26(23):2733‐2738. [DOI] [PubMed] [Google Scholar]
- 10. Farquhar J, Thiemens MH, Jackson T. Atmosphere‐surface interactions on Mars: Δ17O measurements of carbonate from ALH 84001. Science. 1998;280(5369):1580‐1582. [DOI] [PubMed] [Google Scholar]
- 11. Liang MC, Mahata S, Laskar AH, Bhattacharya SK. Spatiotemporal variability of oxygen isotope anomaly in near surface air CO2 over urban, semi‐urban and ocean areas in and around Taiwan. Aerosol Air Qual Res. 2017;17(3):706‐720. [Google Scholar]
- 12. Mahata SK, Bhattacharya CH, Wang MC, Liang MC. Oxygen isotope exchange between O2 and CO2 over hot platinum: An innovative technique for measuring Δ17O in CO2 . Anal Chem. 2013;85(14):6894‐6901. [DOI] [PubMed] [Google Scholar]
- 13. Kim ST, Coplen TB, Horita J. Normalization of stable isotope data for carbonate minerals: Implementation of IUPAC guidelines. Geochim Cosmochim Acta. 2015;158:276‐289. [Google Scholar]