# Correction of spike contribution for strontium isotopic measurement by thermal ionization mass spectrometry: a test for spike-standard mixed solutions

- Chang-sik Cheong
^{1}Email author, - Youn-Joong Jeong
^{1}and - Sung-Tack Kwon
^{2}

**5**:26

https://doi.org/10.1186/s40543-014-0026-1

© Cheong et al.; licensee Springer. 2014

**Received: **17 January 2014

**Accepted: **12 February 2014

**Published: **23 April 2014

## Abstract

### Background

The Rb-Sr isotope system has long been used for radiometric dating and petrogenetic investigation. The concentrations of Rb and Sr could be precisely measured by isotope dilution thermal ionization mass spectrometry combined with chemical purification of these elements. For the simultaneous measurement of Sr isotopic composition and isotope dilution, the contribution from the added spike should be carefully corrected.

### Findings

Reliable ^{87}Sr/^{86}Sr ratios of the spike-standard mixed solutions were obtained using the new mass bias factor calculated on the basis of measured Sr isotopic ratios. This correction yielded reasonable ^{87}Sr/^{86}Sr ratios for overspiked standard solutions whose spike fractions reaching 25 wt.%.

### Conclusions

The correction procedure described in this study shows that the simultaneous measurement of Sr isotopic composition and isotope dilution is available for the case that the spike proportion in the sample-spike mixture is significantly high (^{84}Sr/^{86}Sr > 3.7). The principle of this correction protocol can also be applied to other isotope systems such as Sm-Nd and Lu-Hf pairs.

## Keywords

## Findings

### Introduction

Rubidium-87 decays to stable ^{87}Sr by emission of β^{−} particle with a decay constant of 1.420 (±0.010) × 10^{−11} years^{−1} (Steiger and Jäger [1977]) which corresponds to a half-life of 48.8 × 10^{9} years. It is notable that this International Union of Geological Sciences-accepted decay constant is being considered to be high by 1% to 2% as summarized in Begemann et al. ([2001]). Rubidium and strontium belong to the groups IA and IIA, respectively. They are easily fractionated from each other through geological processes such as partial melting and igneous and metamorphic mineral growth. Therefore, the ^{87}Rb-^{87}Sr isotope system has long been used for radiometric dating and petrogenetic investigation (Faure and Mensing [2005]).

The traditional thermal ionization mass spectrometry (TIMS) is still regarded as the benchmark technique to measure Rb-Sr isotope ratios. By TIMS, the inter-elemental ratio cannot be directly measured but is obtained through isotope dilution (Moore et al. [1973]), a method of analyzing chemical substances by the addition of isotopically enriched spike to the sample. Considering the inhomogeneous distribution of Rb and Sr in most geological samples, simultaneous measurement of Sr isotopic composition and isotope dilution is essential. In this case, inevitable contribution from the spike should be carefully corrected.

This study evaluates the effectiveness of correction protocol to measure ^{87}Sr/^{86}Sr ratio in a series of mixture of ^{84}Sr-enriched spike and standard solution. It has been tested whether a reasonable ^{87}Sr/^{86}Sr ratio could be obtained for overspiked standard solutions of which spike fractions reach 45 wt.%.

## Availability and requirements

### Preparation of spike and standard solution

The ^{84}Sr-enriched isotope spike and standard solutions were prepared at the Korea Basic Science Institute (KBSI) in Ochang. In the following, all errors are quoted on the basis of 2 *σ* standard error, unless stated otherwise.

The spike, SrCO_{3} form, was provided by the Oak Ridge National Laboratory (batch number = 236,201, order number = 65-0056). It was dissolved in hot 10% HNO_{3} and diluted to about 15 μg/g solution with 5% HNO_{3}. The AnApure^{TM} ICP standard of 1,002 (±10) mg/L Sr (lot no. AEP-130-726) was diluted to 21.480 μg/g solution in 2% HNO_{3} (the specific gravity of 2% HNO_{3} = 1.028 g/mL) and then was admixed with the spike solution. Ten mixed solutions were prepared with mixing proportions (spike/standard) ranging from about 1:1.2 to 1:70 in weight.

### Instrumental analysis

The Rb-Sr isotopic analysis was conducted by using a Phoenix (Isotopx) TIMS, Cheshire, CW, UK, installed at the KBSI. This instrument is equipped with eight movable Faraday collectors and one fixed axial channel where the ion beam intensities can be measured with either a Faraday collector or an ion counting Daly detector.

In this study, all required isotopes were simultaneously detected on Faraday collectors. The sensitivity on ^{88}Sr was typically around 3 V (10^{11} Ω resistors). The strontium isotope measurements of the standard and spike-standard mixed solutions were performed with a multi-dynamic mode (Lenz and Wendt [1976]) in which the Faraday collectors were set to simultaneously detect ^{84}Sr (axial), ^{86}Sr (H2), ^{87}Sr (H3), and ^{88}Sr (H4) for the first static run, and ^{84}Sr (L2), ^{86}Sr (H1), ^{87}Sr (H2), and ^{88}Sr (H3) for the second run. One measurement consists of 5 blocks of 12 cycles with an integration time of 10 s. The mass bias was exponentially normalized to ^{86}Sr/^{88}Sr = 0.1194. The mean multi-dynamic ^{87}Sr/^{86}Sr acquired for NBS987 was 0.710252 ± 0.000007 (*n* = 7) during the course of this study.

The isotopic composition of ^{84}Sr-enriched spike was measured with a multi-static mode (100 cycles, 5 blocks, integration time = 10 s) in which the Faraday collectors were set to detect ^{84}Sr (axial), ^{86}Sr (H2), ^{87}Sr (H3), and ^{88}Sr (H4). In this measurement, the instrumental mass fractionation was not normalized.

### Results and discussion

Five measurements for the ^{84}Sr spike yielded an average ^{84}Sr/^{88}Sr of 561.4 ± 0.9, ^{86}Sr/^{88}Sr of 0.7661 ± 0.0010, and ^{87}Sr/^{88}Sr of 0.1819 ± 0.0030, respectively. Therefore, the ^{84}Sr enrichment and atomic weight of the spike are calculated to be 83.9242 and 99.65 at.%, respectively. Although the instrumental mass fractionation was not corrected during the TIMS measurement, this enrichment value is well matched with the suggested value (99.64 ± 0.01%, Tracy [1999]). The exponentially normalized multi-dynamic measurement of the Sr standard yielded an average ^{87}Sr/^{86}Sr ratio of 0.707630 ± 0.000009 (*n* = 5).

^{86}Sr/

^{88}Sr = 0.1194. This mass bias correction is not valid because the

^{86}Sr/

^{88}Sr of the added spike was significantly shifted from the natural value through the enrichment processes from 0.1194 to 0.7661. The first step for the correction of spike contribution is to determine a new mass bias factor (

*α*

_{new}) from the measured Sr isotope ratios. In the following, ‘

*s*’ denotes the normal Sr standard, ‘

*t*’ denotes the Sr spike, and ‘

*m*’ and ‘

*c*’ represent the measured and corrected values, respectively. The (86

*t*/86

*s*) can be calculated using (84/86)

*m*, (84/86)

*s*, and (84/86)

*t*:

Because the measured 84/86 ratio used in the above calculation has an uncertainty due to incorrect normalization to 86/88 = 0.1194, the 86*t*/86*s* should be recalculated after determination of the new mass bias factor (see below).

*s*can be reduced by using (86/88)

*m*, (88

*t*/88

*s*), and (86/88)

*t*:

*s*. The exponential law (Russel et al. [1978]) yields a mass bias factor before (

*α*

_{old}) and after (

*α*

_{new}) the spike correction as the following:

*M*’ denotes the mass of the isotope.

The newly corrected (84/86) ratios of the ten mixed solutions yielded a mean Sr concentration of 15.271 ± 0.031 μg/g for the ^{84}Sr-enriched spike prepared in this study.

*c*can be newly calculated using measured Sr isotope ratios as the following.

Finally, the (87/86)*c*(new) is used for the calculation of the (87/86)*s*:${\left(\frac{87}{86}\right)}_{\mathit{s}}={\left(\frac{87}{86}\right)}_{\mathit{c}\phantom{\rule{0.24em}{0ex}}\left(\mathrm{new}\right)}\times \left(1+\frac{{86}_{\mathit{t}}}{{86}_{\mathit{s}}}\right)-{\left(\frac{87}{86}\right)}_{\mathit{t}}\times \frac{{86}_{\mathit{t}}}{{86}_{\mathit{s}}}$ because ${\left(\frac{87}{86}\right)}_{\mathit{m}}\phantom{\rule{0.5em}{0ex}}=\phantom{\rule{.5em}{0ex}}\frac{{87}_{\mathit{s}}+{87}_{\mathit{t}}}{{86}_{\mathit{s}}+{86}_{\mathit{t}}}\phantom{\rule{.5em}{0ex}}=\phantom{\rule{.5em}{0ex}}\frac{\frac{{87}_{\mathit{s}}}{{86}_{\mathit{s}}}+\frac{{87}_{\mathit{t}}}{{86}_{\mathit{s}}}}{1+\frac{{86}_{\mathit{t}}}{{86}_{\mathit{s}}}}\phantom{\rule{.5em}{0ex}}=\phantom{\rule{.5em}{0ex}}\frac{{\left(\frac{87}{86}\right)}_{\mathit{s}}+\frac{{86}_{\mathit{t}\phantom{\rule{0.25em}{0ex}}}}{{86}_{\mathit{s}}}\times {\left(\frac{87}{86}\right)}_{\mathit{t}}\phantom{\rule{0.25em}{0ex}}}{1+\frac{{86}_{\mathit{t}}}{{86}_{\mathit{s}}}}$ (it is noted that 86_{t}/86_{s} can be recalculated on the basis of newly corrected 84/86).

^{87}Sr/

^{86}Sr ratios of the mixed solutions are displayed in Figure 1 with the measured values of the unspiked standard. As shown in Figure 1, the protocol described in this study successfully corrected the spike contribution in the case that the spike fraction in the mixture reaches 25 wt.% (

^{84}Sr/

^{86}Sr

_{mixture}> 3.7). It is not clear why the corrected

^{87}Sr/

^{86}Sr ratio for mix 1 solution (spike fraction = 45.1 wt.%) deviates from the unspiked standard value. The corrected

^{87}Sr/

^{86}Sr ratios of nine mixed solutions (mix 2 to mix 10) yield an indistinguishable average of 0.707633 ± 0.000010 from the unspiked value (0.707630 ± 0.000009). There is no trend between the corrected

^{87}Sr/

^{86}Sr and the spike fraction (or

^{84}Sr/

^{86}Sr

_{mixture}) in the range from 1.4 to 25.9 wt.%. It is noted that the principle of this correction protocol can also be applied to other isotope systems such as Sm-Nd and Lu-Hf pairs, as briefly interpreted in the study of Cheong and Kwon ([2010]).

**Correction results for the spike-standard mixed solutions**

86/88 | % SE | 84/86 | % SE | 84/86 | 87/86 | % SE | 87/86 | 2 | Spike wt.% | |
---|---|---|---|---|---|---|---|---|---|---|

Mix 1 | 0.12090 | 0.0068 | 8.4583 | 0.0050 | 8.5427 | 0.705574 | 0.0011 | 0.707582 | 0.000016 | 45.1 |

Mix 2 | 0.12034 | 0.0089 | 3.6918 | 0.0094 | 3.7076 | 0.706777 | 0.0009 | 0.707634 | 0.000013 | 25.9 |

Mix 3 | 0.12030 | 0.0048 | 2.4858 | 0.0051 | 2.4929 | 0.707068 | 0.0010 | 0.707640 | 0.000014 | 18.9 |

Mix 4 | 0.12032 | 0.0049 | 1.9667 | 0.0050 | 1.9711 | 0.707165 | 0.0009 | 0.707615 | 0.000013 | 15.5 |

Mix 5 | 0.11982 | 0.0179 | 1.5658 | 0.0187 | 1.5686 | 0.707292 | 0.0010 | 0.707644 | 0.000014 | 12.6 |

Mix 6 | 0.12016 | 0.0016 | 1.2043 | 0.0022 | 1.2059 | 0.707349 | 0.0010 | 0.707618 | 0.000014 | 9.9 |

Mix 7 | 0.11983 | 0.0034 | 0.7787 | 0.0030 | 0.7794 | 0.707469 | 0.0008 | 0.707638 | 0.000011 | 6.5 |

Mix 8 | 0.11976 | 0.0143 | 0.4234 | 0.0147 | 0.4236 | 0.707568 | 0.0010 | 0.707653 | 0.000014 | 3.4 |

Mix 9 | 0.12023 | 0.0185 | 0.2831 | 0.0103 | 0.2832 | 0.707593 | 0.0010 | 0.707646 | 0.000014 | 2.1 |

Mix 10 | 0.11983 | 0.0145 | 0.2071 | 0.0173 | 0.2072 | 0.707575 | 0.0010 | 0.707610 | 0.000014 | 1.4 |

Average | 0.707633 | |||||||||

SD | 0.000015 | |||||||||

2 | 0.000010 |

## Declarations

### Acknowledgements

This study was supported by the KBSI grant (G34200).

## Authors’ Affiliations

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## Copyright

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