Shitou
Wu
*ab,
Dingshuai
Xue
ab,
Yueheng
Yang
ab,
Hao
Wang
ab,
Chunlai
Li
c and
Fuyuan
Wu
ab
aState Key Laboratory of Lithospheric and Environmental Coevolution, Institute of Geology and Geophysics, Chinese Academy of Sciences, Beijing, 100029, P.R. China. E-mail: shitou.wu@mail.iggcas.ac.cn
bCollege of Earth and Planetary Science, University of Chinese Academy of Sciences, Beijing, 100049, P.R. China
cKey Laboratory of Lunar and Deep Space Exploration, National Astronomical Observatories, Chinese Academy of Sciences, 100101, Beijing, P.R. China
First published on 31st October 2024
The bulk chemical compositions of extraterrestrial materials can provide critical information on the evolution and magmatism of planetary bodies. However, accurate measurements are challenging because these samples, particularly returned samples, are extremely limited and valuable. We demonstrate the practicality of chemical analysis using laser ablation-inductively coupled plasma-mass spectrometry (LA-ICP-MS) on highly diluted fused glass discs (lithium borate flux:sample = 100:1). Only 30 mg of sample is required to produce a lithium borate disc, which is one magnitude lower than previously used (>300 mg). We proposed a modified Jet sample cone (the orifice diameter enlarging from 1.1 mm to 1.2 mm) to improve the sensitivity by a factor of ∼4.5 compared to that of standard sample cone. The interferences from the lithium borate discs were evaluated systemically, and corrections are necessary for some elements (e.g., Si, Ca, Pb). The limits of detection for most elements are in the range of 0.1–1.0 μg g−1. The analytical precision is better than 30% (relative standard deviation) for elements with concentrations of >0.5 μg g−1. The accuracy is better than 15% (relative deviation), as demonstrated by analyses of BCR-2 and BHVO-1 rock powder reference materials. This innovative technique was applied to lunar samples collected by Chang'e-5 (CE-5) mission, and an independent dataset of 38 major and trace elements was obtained. We report the average chemical composition of the CE-5 lunar soil samples, which will be an important reference for future study. This method will be useful for other precious extraterrestrial samples (e.g., CE-6 lunar samples).
The introduction of ICP-MS to geochemistry and cosmochemistry fields in the 1980s led to more elemental data being reported for extraterrestrial materials.8 The advantages of ICP-MS are low detection limits (sub-ng g−1 level), the ability of multiple element analyses, and high analysis efficiency, making it as the most popular technique for multiple element analyses. However, this technique generally requires 50–100 mg of sample and uses acid digestion to dissolve powders, inevitably destroying the sample. Although previous studies attempted to reduce the sample size to <50 mg using low-dilution ratio and highly sensitive ICP-MS, it is still not able to avoid destroying the samples and may suffer from matrix effects due to the high salinity effect.4 Another issue faced by ICP-MS is the instability or adsorption of high field strength elements (e.g., Ta) in acid solutions, leading to inaccurate results for these elements.9
Laser ablation (LA)-ICP-MS is another technique for measuring bulk chemical compositions, which requires converting samples to homogeneous solid state materials (e.g., glass and powder pellets).10–19 Flux-free fusion leads to less contamination, but it may be affected by the loss of volatile elements (e.g., Pb) during the high temperature melting (>1500 °C).15,17 In addition, flux-free fusion is not able to produce homogeneous glasses for ultramafic rocks (e.g. CE-5 basalt, SiO2 < 47%).20 The addition of flux is necessary to avoid mineral crystallization during the rapid cooling of the melt. Lithium borate is a commonly used flux. Traditionally, the flux:sample ratio is in a range of 3:1–10:1. This dilution factor requires 300–1250 mg of sample, which is cleatly a large amount for valuable samples.
In this study, we firstly demonstrate the practicality of chemical analysis using LA-ICP-MS on highly diluted fused glass discs (flux:sample = 100:1). Only 30 mg of sample is required to produce the standard lithium borate discs (for XRF analysis). The sample size could be down to sub-mg levels with the proportionally reduced flux. The challenges of LA-ICP-MS analysis on such highly diluted fused glass discs are: (1) requirement of high sensitivity due to the low sample proportion (∼1%); (2) identification and correction of interferences. The Jet sample cone was modified with the orifice diameter enlarging from 1.1 mm to 1.2 mm, leading to ∼4.5 fold sensitivity improvement compared to that using standard sample cone. We systematically evaluated the interferences from lithium borate discs, and corrections are necessary for some elements (e.g., Si, Ca, Pb). The analytical precision and accuracy were evaluated using the BCR-2 and BHVO-1 rock powder reference materials. We then applied this method to the Chang'e-5 (CE-5) lunar soil sample and obtained an independent chemical concentration dataset for 38 elements.
Fig. 1 Photographs of (a) CE-5 lunar soil samples and (b) the highly diluted lithium borate disc used for LA-ICP-MS analysis. |
Fig. 2a shows the intensities of the 139La and 238U signals using the standard cone, Jet cone and modified Jet cone, indicating ∼4.5-fold sensitivity improvement. Such improved sensitivity is helpful for the LA-ICP-MS analysis in highly diluted fused glass discs. The limits of detections (LODs) of 38 elements were calculated following Pettke et al.34 (Fig. 2b; ESI Table S3†). The LODs using the modified Jet cone are clearly better than those using the standard cone (Fig. 2b). In general, the LODs of most trace elements are in a range of 0.1–1.0 μg g−1. The light elements have higher LODs than heavy elements. The detection capability of our analytical protocol is enough for CE-5, BCR-2 and BHVO-1 samples (Fig. 2b).
Fig. 2 (a) Maximum 137La and 238U intensities using standard, Jet, and modified Jet sample cones in Ar plasma while maintaining a Th+/U+ ratio of 0.9–1.1 and ThO+/Th+ ratio of <0.5%. The sample is NIST SRM 612 with laser parameters of 50 μm spot size, 5 Hz frequence, and 3.0 J cm−2 energy density. (b) Limits of detections (LODs) of the 38 elements calculated using the protocol of Pettke et al. (2012)34 using the modified Jet cones and “LOD_s” represents the values using standard cones. The compositions of BCR-2, BHVO-1, and CE-5 are shown for comparison. |
These interferences must be identified and cottected before obtaining high quality data. Isotopes affected by impurities in the flux reagent include 29Si, 43Ca, 60Ni, 65Cu, 66Zn, and 137Ba. Contamination affects mainly 208Pb (ESI Fig. S2†). In general, the lithium borate discs are clean, and only a few elements (Al, Si, P, Ca, Ti, and V) have contents higher than 10 μg g−1; however, these interferences could greatly affect the accuracy due to the high dilution of the fused glass discs. For example, the P interference from lithium borate discs on the sample is about 1000 μg g−1, which could not be effectively corrected for the CE-5 lunar sample, while Si, Fe, Ti, Mg, Cr, and Mn could be effectively corrected. ESI Fig. S3† compares the interference-corrected and uncorrected SiO2 results, indicating such corrections are necessary to obtain the accurate data. The recommended approach is measuring the minor and trace elements in blank flux discs and subtracting those values from each analysis of the lunar soil sample.
Samples | CE5C0400 | CE5C0800 | CE5C0800 | CE5C0800 | Overall mean | |||||
---|---|---|---|---|---|---|---|---|---|---|
Techniques | ICP-MS | INAA | XRF | LA-ICP-MS | ||||||
Values | 2SD | Values | 2SD | Values | 2SD | Values | 2SD | Values | 2SD | |
n = 7 | n = 1 | n = 1 | n = 1 | |||||||
SiO2 | — | — | — | — | 42.2 | 0.3 | 42.3 | 1.0 | 42.3 | 0.3 |
TiO2 | 5.12 | 0.14 | 5.19 | 0.03 | 5.00 | 0.06 | 4.97 | 0.36 | 5.07 | 0.21 |
Al2O3 | 11.6 | 0.2 | 10.8 | 0.5 | 10.8 | 0.2 | 10.6 | 0.7 | 10.9 | 0.8 |
FeO | 22.7 | 0.9 | 22.0 | 0.9 | 22.5 | 0.3 | 22.7 | 1.8 | 22.5 | 0.7 |
MnO | 0.280 | 0.010 | 0.278 | 0.011 | 0.280 | 0.030 | 0.303 | 0.022 | 0.285 | 0.024 |
MgO | 6.52 | 0.29 | 6.40 | 0.41 | 6.48 | 0.35 | 6.26 | 0.46 | 6.42 | 0.23 |
CaO | 11.6 | 0.3 | 10.4 | 0.7 | 11.0 | 0.1 | 11.0 | 0.7 | 11.0 | 1.0 |
Na2O | 0.460 | 0.010 | 0.461 | 0.028 | 0.26 | 0.21 | — | — | 0.39 | 0.23 |
K2O | 0.210 | 0.010 | 0.182 | 0.018 | 0.19 | 0.15 | 0.179 | 0.017 | 0.190 | 0.028 |
P2O5 | 0.270 | 0.020 | — | — | 0.230 | 0.050 | — | — | 0.250 | 0.057 |
Li | 15.4 | 0.6 | — | — | — | — | — | — | 15.4 | 0.6 |
Be | 2.84 | 0.11 | — | — | — | — | — | — | 2.84 | 0.11 |
K | 1510 | 166 | 1510 | 151 | — | — | 1480 | 125 | 1500 | 32 |
Sc | 62.9 | 3.6 | 66.0 | 2.6 | — | — | 72.1 | 9.6 | 67.0 | 9.4 |
Mn | 2150 | 170 | 2150 | 86 | — | — | 2350 | 150 | 2220 | 225 |
Co | 37.2 | 1.6 | 40.0 | 1.6 | — | — | 44.7 | 6.3 | 40.6 | 7.6 |
Ni | 139 | 26 | 136 | 11 | — | — | 139 | 57 | 138 | 4 |
Cu | 12.2 | 2.2 | — | — | — | — | — | — | 12.2 | 2.2 |
Zn | 14.2 | 0.8 | 16.2 | 3.2 | — | — | — | — | 15.2 | 2.8 |
Ga | 5.79 | 0.38 | — | — | — | — | 5.8 | 2.9 | 5.79 | 0.01 |
Rb | 5.23 | 0.60 | 7.5 | 1.5 | — | — | 4.3 | 1.5 | 5.7 | 3.3 |
Sr | 313 | 18 | 276 | 22 | — | — | 328 | 21 | 306 | 53 |
Y | 116 | 12 | — | — | — | — | 102 | 6 | 109 | 20 |
Zr | 545 | 50 | 458 | 34 | — | — | 503 | 29 | 502 | 87 |
Nb | 35.6 | 3.8 | — | — | — | — | 30.9 | 2.6 | 33.3 | 6.6 |
Cs | 0.220 | 0.020 | 0.169 | 0.038 | — | — | 0.16 | 0.19 | 0.181 | 0.069 |
Ba | 395 | 46 | 362 | 35 | — | — | 415 | 34 | 391 | 53 |
La | 35.4 | 4.0 | 36.1 | 1.4 | — | — | 34.4 | 2.8 | 35.3 | 1.7 |
Ce | 99 | 11 | 92.8 | 3.7 | — | — | 79.2 | 4.9 | 90 | 20 |
Pr | 12.7 | 1.6 | 12.5 | 2.2 | — | — | 11.8 | 1.3 | 12.3 | 0.9 |
Nd | 59.3 | 7.0 | 58.4 | 5.8 | — | — | 56.2 | 5.9 | 58.0 | 3.2 |
Sm | 17.0 | 1.8 | 16.1 | 0.6 | — | — | 16.7 | 3.8 | 16.6 | 0.9 |
Eu | 2.77 | 0.20 | 2.56 | 0.10 | — | — | 2.69 | 0.67 | 2.67 | 0.21 |
Gd | 19.6 | 2.0 | 18.9 | 0.8 | — | — | 19.9 | 3.3 | 19.5 | 1.1 |
Tb | 3.27 | 0.36 | 3.51 | 0.28 | — | — | 3.16 | 0.43 | 3.31 | 0.36 |
Dy | 20.5 | 2.2 | 20.9 | 1.4 | — | — | 20.4 | 2.9 | 20.6 | 0.5 |
Ho | 4.07 | 0.46 | 4.50 | 1.40 | — | — | 4.04 | 0.65 | 4.20 | 0.51 |
Er | 11.3 | 1.2 | — | — | — | — | 11.4 | 1.8 | 11.3 | 0.1 |
Tm | 1.57 | 0.18 | 0.800 | 0.040 | — | — | 1.54 | 0.42 | 1.30 | 0.87 |
Yb | 9.90 | 0.76 | 9.49 | 0.57 | — | — | 9.6 | 2.5 | 9.65 | 0.44 |
Lu | 1.36 | 0.14 | 1.41 | 0.08 | — | — | 1.39 | 0.37 | 1.39 | 0.05 |
Hf | 14.0 | 1.6 | 13.6 | 0.5 | — | — | 14.3 | 3.5 | 14.0 | 0.7 |
W | 0.50 | 0.14 | 0.79 | 0.24 | — | — | — | — | 0.65 | 0.41 |
Ta | 1.83 | 0.14 | 1.77 | 0.24 | — | — | 1.57 | 0.42 | 1.72 | 0.27 |
Pb | 1.89 | 0.20 | — | — | — | — | 1.35 | 0.70 | 1.62 | 0.76 |
Th | 5.14 | 0.56 | 4.72 | 0.28 | — | — | 5.00 | 0.71 | 4.95 | 0.43 |
U | 1.35 | 0.16 | 1.41 | 0.28 | — | — | 1.15 | 0.28 | 1.30 | 0.27 |
The CE-5 lunar sample has an Rb content of ∼5.0 μg g−1, higher than the LODs of the three techniques; therefore, the large variation may suggest that Rb is heterogeneous in the CE-5 samples. The Cs and W data also show large scatter, which is probably related to the low contents of those elements. The slight scatter in Pb contents is probably due to the contamination issue of ICP-MS and LA-ICP-MS. It should be noted that the Tm content determined by INAA is clearly lower than that determined by ICP-MS and LA-ICP-MS. The reason for this is unclear, but it may be related to analytical issues with the INAA technique. In general, the data presented in this study further support the conclusion that the CE-5 lunar soil samples are homogeneous with only a few volatile elements showing slight heterogeneity.
Although the sample size used in this study is 30 mg (this size is required for the XRF standard glass disc), the amount of sample size could be down to sub-mg levels with proportionally reduced flux. The highly diluted fused glass discs transform samples from their original state to glass, but this glass disc can be long-term and low-cost preserved for future usage. In addition, it is practically to carry out isotopic ratio measurements (e.g. U) in these glass discs using LA-MC-ICP-MS and SIMS. Our method could yield precise major element concentration data that are comparable to XRF analysis (Table 1). The main drawback of this technique is the interferences from the flux and contamination during preparation, particularly Li and B, implying that these elements cannot be analyzed. Future study may be focusing on the purification of Li–B flux or selection of other fluxes.
With the new data reported in this study, the average chemical composition of the CE-5 lunar soil sample could be calculated. The dataset was obtained for the samples from different batches (CE5C0400, CE5C0600, and CE5C0800) using different methods (solution ICP-MS, INAA, XRF, and LA-ICP-MS; Table 1). Further interpretation of these data is outside of the scope of this study. However, the mean data reported here could represent the bulk compositions of the CE-5 lunar soils, and it will be an important reference for the future studies.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4ja00329b |
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