Chao-Feng
Li
*ab,
Zhu-Yin
Chu
ab and
Peng
Peng
ab
aState Key Laboratory of Lithospheric Evolution, Institute of Geology and Geophysics, Chinese Academy of Sciences, Beijing 100029, China. E-mail: cfli@mail.iggcas.ac.cn; Tel: +86-10-82998583
bInnovation Academy for Earth Science, Chinese Academy of Sciences, Beijing 100029, China
First published on 25th November 2025
Sn is the main isobaric interferent for Cd isotopic composition determination. To eliminate Sn, two-step separation methods using an anion resin combined with commercially available TRU and UTEVA extraction resins are usually required for high-precision Cd isotope ratio measurements. First, the AG1-X8 or AGMP-1M anion resin is utilized to eliminate the matrix and most Sn isobaric interferences. Subsequently, extraction resins are employed to eliminate residual Sn. However, these extraction resins are costly. In this study, we present a new approach using the commercially available TBP (tri-n-butyl phosphate) extraction resin as an alternative. The TBP extraction resin is highly cost-effective (∼5% of the cost of TRU or UTEVA extraction resins) and shows excellent performance in Sn removal. Our two-step procedure achieves high recovery (>99% Cd) with a low procedural blank (<30 pg), enabling the efficient isolation of Sn and Cd from bulk rock solutions. The validity of the proposed method was confirmed by analyzing six geological reference materials, including GSD-11 with a very high Sn/Cd ratio, yielding results in good agreement with the published values.
Effective Cd sample preparation5–8,14–33 is a precondition for achieving accurate and precise Cd isotopic data for geological, biological, and environmental materials, as isobaric interferences give rise to wrong analytical data in both TIMS and MC-ICP-MS. Incomplete isolation of Cd from Pd, In, and Sn may lead to significant isobaric interferences, such as 106Pd+ on 106Cd+, 108Pd+ on 108Cd+, 110Pd+ on 110Cd+, 112Sn+ on 112Cd+, 113In+ on 113Cd+, 114Sn+ on 114Cd+, and 116Sn+ on 116Cd+. Single-column techniques based on AG1-X8 or AGMP-1M anion-exchange resins are very effective in removing matrix elements (K, Na, Ca, Mg, Al, Fe, Ti, and Mn) as well as In and Pd isobaric interferences, but they cannot completely eliminate Sn isobaric interference, with 2–5% of Sn co-eluting with the Cd fraction.5,31 To completely eliminate Sn isobaric interference, current Cd purification strategies mainly adopt two-step separation schemes combining the anion-exchange resin and extraction resin techniques, which can be roughly classified into four categories (I) Using the TRU extraction resin12,13,26 to eliminate Sn after purification by the AG1-X8 or AGMP-1M anion resin (II) Using the UTEVA extraction resin30 to eliminate Sn after purification by the AG1-X8 or AGMP-1M anion resin (III) Employing the BPHA (N-benzoyl-N-phenylhydroxylamine) extraction resin28 to eliminate Sn after purification by the AG1-X8 or AGMP-1M anion resin (IV) employing repeated anion exchange resin separation with AG1-X8 (ref. 31) or AGMP-1 M20,32 to remove Sn.
Although existing methods achieved high Cd recoveries (>90%) and low Cd blanks (<0.15 ng), they typically require relatively large volumes of eluent and numerous evaporation/transfer steps, which prolong the separation process and increase analytical costs.
This study aims to develop a rapid and cost-effective Cd separation scheme based on the AG1-X8 and TBP (tri-n-butyl phosphate) extraction resin for determining Cd isotopes using DS-TIMS. The TBP resin exhibits a comparable capability to commercially available TRU and UTEVA Spec resins in separating Cd from Sn, but its cost is only ∼5% that of these extraction resins, amounting to only ∼0.15 U.S dollars per separation. The reliability and accuracy of the proposed method were validated using synthetic solutions with high Sn/Cd ratios and geological reference materials.
AG1-X8 anion resin column: 7 cm long × 6 mm i.d. With a 5 mL reservoir, packed with the Bio-Rad AG1-X8 resin (200–400 mesh), and 1 mL of resin bed volume.
TBP extraction resin column: 6 cm long × 4 mm i.d. With a 2 mL reservoir, packed with the TBP resin (80–120 mesh) purchased from Beijing Realkan Separation Technology Co., Ltd. (https://realkan.cn/Products_d/10.html), and 0.13 mL of resin bed volume. The TBP extraction resin was pre-cleaned by shaking it with Millipore water and 6 mol per L HCl in sequence. This was repeated 3–4 times (until no more foam appeared), and then the mixture was stored in 1 M HCl.
108Cd-116Cd double spike: The 108Cd–116Cd method reported by Li et al.31 was employed to correct for isotopic fractionation during chemical purification and TIMS measurement.
For the carbonate materials (COQ-1 and JDo-1), approximately 40 ± 0.1 mg of the sample powder was weighed into screw-top PFA vials. The samples were dissolved on a hotplate at 110 °C using 2 mL of 3 M HCl for 4 hours.
These samples contained 23.2–226 ng of Cd, as calculated according to the previously published Cd content in literature.19–22 Then, an appropriate amount of the 108Cd–116Cd double spike was added to each sample solution with a spike/sample mass ratio (3.5) for all samples in this study. These PFA vials were then tightly capped and heated on a hotplate overnight at 120 °C to ensure complete homogenization of the mixed solutions. Finally, the vials were opened, and the sample solutions were evaporated to dryness and then re-dissolved in 1 mL of 6 M HCl.
In this study, as shown in Fig. 1 and Table 1, a two-step resin column was employed to purify Cd. First, the AG1-X8 anion resin chromatography method was employed to remove the matrix and most isobaric interference elements (Table 1), as reported by Li et al.31 After the AG1-X8 column, the collected Cd fractions, containing ∼99.5% of Cd along with ∼2.7% of Sn, were dried down on a hotplate at 120 °C. Subsequently, a small column filled with the TBP extraction resin (0.13 mL, TBP resin, 80–120 mesh) was used to purify Cd to eliminate residual Sn. Before performing TBP column separation, a synthetic mixed standard solution containing 5 µg of Zr, Mo, Cd, Sn, and In was employed to calibrate and optimize the column procedure in order to obtain satisfactory Cd purity. The elemental distribution yield was measured using an iCAP Q-ICP-MS (Thermo Fisher Scientific). The Cd fraction was re-dissolved with 0.3 mL of 6 M HCl for TBP column loading. As shown in Table 1b, the TBP resin column was washed with 2 mL of H2O and conditioned with 2 mL of 6 M HCl. The 0.3 mL Cd sample solution was then loaded onto the TBP column. In 6 M HCl medium, 99.5% of Sn was absorbed on the TBP column, while all Cd was eluted using 3 mL of 6 M HCl. The final Cd fraction was dried down on a hotplate at 150 °C.
| Procedure step | Reagent | Volume (mL) |
|---|---|---|
| a The AG1-X8 and TBP columns were filled with 1 mL of the AG1-X8 resin and 0.13 mL of the TBP resin, respectively. After the two-step column purification, the yield of Cd is approximately 99.4%, and the residual Sn is lower than 0.03%. | ||
| Step Ⅰ (AG1 column) | ||
| Cleaning column | 2 M HNO3 | 10 |
| Cleaning column | Milli-Q water | 10 |
| Cleaning column | 3 M HCl | 3 |
| Loading sample | 6 M HCl | 1 |
| Rinsing matrix | 6 M HCl | 3 |
| Rinsing Fe, In, and Mo | 0.4 M HCl | 12 |
| Rinsing Zn, Sn | 0.5 M HNO3 + 0.1 M HBr | 12 |
| Collecting Cd | 2 M HNO3 | 8 |
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||
| Step II (TBP column) | ||
| Cleaning column | Milli-Q water | 2 |
| Cleaning column | 6 M HCl | 2 |
| Loading sample | 6 M HCl | 0.3 |
| Collecting Cd | 6 M HCl | 3 |
Organic compounds released from resins are known to have a detrimental impact on the sensitivity of isotopic analyses by TIMS.34–37 Minor organics released from the TBP resin, which strongly inhibited the ionization of Cd, were removed by evaporating the Cd fraction on a hotplate at 160 °C, and then, it was digested using 0.5 mL of 14 M HNO3 and 0.1 mL of 11.8 M HClO4 on a 180 °C hotplate for two hours in tightly sealed PFA vials. Subsequently, the sample solution was evaporated to dryness again on a 180 °C hotplate and then treated with 1 mL of 6 M HCl in closed PFA vials on a 160 °C hotplate for two hours for expelling residual HClO4. Finally, the digested Cd sample was dried at 180 °C for TIMS analysis.
The whole procedural blank, encompassing all steps from sample digestion to the final Cd isotopic measurement by TIMS, was 25 ± 5 pg (n = 5), which is negligible compared with the amount of Cd (104–1017 ng, including spike) processed through the columns.
| Element | L3 | L2 | L1 | CC | H1 | H2 | H3 | H4 |
|---|---|---|---|---|---|---|---|---|
| Cd | 108Cd | 110Cd | 111Cd | 112Cd | 113Cd | 114Cd | 116Cd | 117Sn |
For Cd isotope measurements, the Re filament was heated at a rate of 500 mA min−1 until the 114Cd signal reached approximately 10 mV. The ion beam was then roughly focused, and the filament current was gradually increased to produce a typical signal of approximately 500–1500 mV for 114Cd, depending on the sample loading size. Each measurement run consisted of 200 cycles, yielding an internal precision of 0.03–0.05‰ (2SE) for most δ114/110Cd values. The integration time per cycle was 4 seconds. 117Sn was monitored to correct for possible isobaric interference on 114Cd (from 114Sn) and 116Cd (from 116Sn). The 117Sn/112Cd ratios obtained during sample analysis were all <3 × 10−5, indicating that Sn isobaric interferences were negligible. Additionally, 105Pd and 115In peaks were checked in the peak-scan mode prior to data acquisition, and no detectable Pd or In signals were observed, confirming the absence of such interferences.
All data for the geological samples doped with the 108Cd–116Cd double spike were calculated offline following the procedures described by Li et al.31,34,35 for Cd and Cr isotope analysis and by Heuser et al.38 for Ca isotope analysis. The NIST SRM 3108 Cd standard was analyzed to monitor the instrument status. The 114Cd/110Cd ratios for un-spiked NIST SRM 3108 were normalized to 110Cd/112Cd = 0.517
330 for mass fractionation correction using the exponential law.21,31 In this study, 100 ng NIST SRM 3108 standard loads gave a mean 114Cd/110Cd of 2.30429 ± 8 (2SD, n = 8), which is in good agreement with the previously reported value (2.30425 ± 20).21,31
| Fraction | Zr (%) | Mo (%) | Cd (%) | In (%) | Sn (%) | Eluting volume (mL) |
|---|---|---|---|---|---|---|
| a F1–F3 was eluted with 1 M HCl, F4–F6 was eluted with 3 M HCl, and F7–F9 was eluted with 6 M HCl. | ||||||
| F-1 | 75.1 | 42.3 | 61.8 | 51.5 | 0.30 | 0.3 |
| F-2 | 16.7 | 43.7 | 36.2 | 43.4 | 0.30 | 1.5 |
| F-3 | 0.90 | 2.5 | 1.32 | 2.00 | 1.60 | 1.5 |
| Yield% | 92.6 | 88.6 | 99.3 | 96.9 | 2.20 | |
| F-4 | 35.5 | 0.07 | 0.02 | 0 | 0.20 | 0.3 |
| F-5 | 5.40 | 0.04 | 70.9 | 0.50 | 0.17 | 1.5 |
| F-6 | 0.60 | 0.03 | 28.6 | 29.7 | 0.14 | 1.5 |
| Yield% | 41.5 | 0.1 | 99.6 | 30.2 | 0.51 | |
| F-7 | 28.0 | 0.04 | 0.03 | 0.01 | 0.41 | 0.3 |
| F-8 | 1.97 | 0.02 | 72.4 | 0 | 0.32 | 1.5 |
| F-9 | 0.29 | 0.01 | 27.4 | 0.02 | 0.21 | 1.5 |
| Yield% | 30.2 | 0.08 | 99.8 | 0.03 | 0.93 | |
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| Fig. 2 Sorption behavior of Sn, Cd, Mo, In and Zr using the TBP resin column in 1 M, 3 M and 6 M HCl media. | ||
During the second TBP column stage, ∼99.5% of Sn, ∼69.8% of Zr and ∼100% of In and Mo were adsorbed by the TBP resin, while ∼99.8% of Cd was eluted using 6 M HCl. According to the AG1-X8 resin scheme reported previously,31 99.6% of Cd was recovered and 97.6% of Sn was removed during the first AG1-X8 column. Therefore, the combined AG1-X8 and TBP column procedure developed in this study yielded a final Cd recovery of ∼99.4% and reduced residual Sn to ∼0.03%.
To verify the Sn removal efficiency of our methods, two synthetic solutions with a high Sn/Cd ratio (200
:
1), which were much higher than those (5–20) of most natural silicates, were prepared by mixing NIST 3108-Cd or AAS-Cd with Sn. These artificial mixtures contained 200 ng of Cd doped with 40
000 ng of Sn, along with a suitable amount of the 108Cd–116Cd double spike. They were purified using our two-step scheme and measured by TIMS.
As shown in Fig. 3 and Table 4, the external precision of the replicated purified samples (n = 8) is −0.673 ± 0.038‰ (2SD) for AAS and −0.014 ± 0.028‰ (2SD) for NIST 3108, both in good agreement with reference values5,19,25,31,32 within error. This demonstrates that our methods were robust even for samples containing up to 40 µg of Sn. No Sn isobaric interferences were detected, as 117Sn/112Cd was lower than 3 × 10−5 during the TIMS measurements.
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| Fig. 3 δ 114/110Cd values of Sn-doped AAS and NIST 3108 standards with a high Sn/Cd ratio (200) after purification using AG1-X8 and TBP columns. | ||
| CRMs | δ 114/110Cd (‰) | 2SE | CRMs | δ 114/110Cd (‰) | 2SE |
|---|---|---|---|---|---|
| AAS-M-1 | −0.674 | 0.032 | NIST3108-M-1 | −0.030 | 0.022 |
| AAS-M-2 | −0.655 | 0.023 | NIST3108-M-2 | −0.014 | 0.031 |
| AAS-M-3 | −0.700 | 0.031 | NIST3108-M-3 | 0.000 | 0.032 |
| AAS-M-4 | −0.677 | 0.023 | NIST3108-M-4 | −0.030 | 0.022 |
| AAS-M-5 | −0.654 | 0.034 | NIST3108-M-5 | −0.014 | 0.032 |
| AAS-M-6 | −0.698 | 0.033 | NIST3108-M-6 | 0.011 | 0.031 |
| AAS-M-7 | −0.651 | 0.025 | NIST3108-M-7 | −0.019 | 0.033 |
| AAS-M-8 | −0.678 | 0.024 | NIST3108-M-8 | −0.013 | 0.025 |
| Mean ± 2SD | −0.673 | 0.038 | Mean ± 2SD | −0.014 | 0.028 |
800 ng of Sn and only 29.6 ng of Cd, making it an ideal test case and a sensitive indicator for assessing the Sn removal effect of our method. Throughout the GSD-11 measurements, no detectable 117Sn signal was observed. As shown in Table 5 and Fig. 4, fifteen replicated analyses of GSD-11 in this study yielded a value of −0.307 ± 0.052‰ (2SD), which is consistent with the average value (−0.304 ± 0.054‰) calculated from the previously published literature.17,20,23,25,32
| CRMs | δ 114/110Cd (‰) | 2SE | Cd ppm | δ 114/110Cd (‰) |
|---|---|---|---|---|
| a The Cd sample size calculated according to the references is estimated to be 226 ng for NOD P-1 (10 mg digestion), 76 ng for NOD A-1 (10 mg digestion), 43 ng for GSS-1a (10 mg digestion), 29.6 ng for GSD-11 (40 mg digestion), 23.2 ng for JDo-1 (40 mg digestion), and 24 ng for COQ-1 (40 mg digestion). | ||||
| GSD-11 | −0.284 | 0.021 | 0.74 (ref. 20) | −0.274 ± 0.037 (ref. 20) |
| Sediment | −0.378 | 0.051 | −0.305 ± 0.054 (ref. 17) | |
| −0.313 | 0.032 | −0.34 ± 0.06 (ref. 23) | ||
| −0.291 | 0.024 | −0.281 ± 0.059 (ref. 32) | ||
| −0.300 | 0.023 | −0.32 ± 0.067 (ref. 25) | ||
| −0.290 | 0.032 | |||
| −0.309 | 0.034 | |||
| −0.342 | 0.063 | |||
| −0.296 | 0.031 | |||
| −0.282 | 0.032 | |||
| −0.273 | 0.032 | |||
| −0.325 | 0.041 | |||
| −0.307 | 0.033 | |||
| −0.311 | 0.034 | |||
| −0.302 | 0.031 | |||
| Mean ± 2SD | −0.307 ± 0.052 | −0.304 ± 0.054 | ||
| NOD A-1 | 0.146 | 0.042 | 7.6 (ref. 21) | 0.12 ± 0.046(ref. 21) |
| Mn nodule | 0.182 | 0.044 | 0.16 ± 0.10(ref. 18) | |
| 0.185 | 0.025 | 0.127 ± 0.035(ref. 22) | ||
| 0.22 ± 0.02(ref. 5) | ||||
| 0.184 ± 0.057(ref. 29) | ||||
| 0.08 ± 0.02(ref. 23) | ||||
| 0.124 ± 0.067(ref. 20) | ||||
| 0.193 ± 0.047(ref. 28) | ||||
| −0.07 (ref.14) | ||||
| 0.15 ± 0.036(ref. 31) | ||||
| 0.112 ± 0.224(ref. 33) | ||||
| Mean ± 2SD | 0.171 ± 0.042 | 0.127 ± 0.154 | ||
| GSS-1a | 0.012 | 0.051 | 4.3 (ref. 19) | 0.11 ± 0.05(ref. 19) |
| Asoil | 0.068 | 0.082 | 0.14 ± 0.10(ref. 23) | |
| −0.068 | 0.032 | 0.11 ± 0.06(ref. 18) | ||
| −0.078 ± 0.05 (ref. 29) | ||||
| 0.098 ± 0.027(ref. 20) | ||||
| 0.08 ± 0.23(ref. 14) | ||||
| 0.099 ± 0.054(ref. 25) | ||||
| 0.01 ± 0.058(ref. 31) | ||||
| Mean ± 2SD | 0.004 ± 0.138 | 0.071 ± 0.142 | ||
| NOD P-1 | 0.147 | 0.042 | 22.6 (ref. 21) | 0.14 ± 0.07(ref. 21) |
| Mn nodule | 0.157 | 0.023 | 0.16 ± 0.03(ref. 30) | |
| 0.182 | 0.025 | 0.16 ± 0.10(ref. 18) | ||
| 0.133 ± 0.038(ref. 20) | ||||
| 0.135 ± 0.074(ref. 22) | ||||
| 0.16 ± 0.04(ref. 26) | ||||
| 0.185 ± 0.048(ref. 29) | ||||
| 0.196 ± 0.073(ref. 28) | ||||
| 0.12 ± 0.04(ref. 23) | ||||
| 0.163 ± 0.04(ref. 19) | ||||
| 0.13 (ref. 14) | ||||
| 0.131 ± 0.169r(ref. 33) | ||||
| 0.165 ± 0.028(ref. 31) | ||||
| Mean ± 2SD | 0.162 ± 0.036 | 0.152 ± 0.046 | ||
| COQ-1 | 0.083 | 0.062 | 0.60 (ref. 19) | 0.098 ± 0.052(ref. 19) |
| Carbonate | 0.099 | 0.066 | 0.143 ± 0.053(ref. 29) | |
| 0.152 | 0.063 | 0.230 ± 0.02(ref. 5) | ||
| 0.123 ± 0.048(ref. 28) | ||||
| 0.113 ± 0.082(ref. 31) | ||||
| Mean ± 2SD | 0.111 ± 0.072 | 0.141 ± 0.104 | ||
| JDo-1 | 0.119 | 0.062 | 0.58 (ref. 22) | 0.002 ± 0.022(ref. 22) |
| Carbonate | 0.125 | 0.076 | 0.080 ± 0.03(ref. 7) | |
| 0.014 | 0.052 | 0.067 ± 0.06(ref. 31) | ||
| Mean ± 2SD | 0.086 ± 0.132 | 0.050 ± 0.082 | ||
For the other five reference materials (NOD P-1, NOD A-1, COQ-1, JDo-1 and GSS-1a), three replicates were conducted for different digestions of the powder materials. All average values of δ114/110Cd showed good agreement within uncertainty, indicating that the precision and accuracy of our separation method were robust and accurate. The Cd amounts shown in Table 5 were estimated according to the sample weights and previously published Cd concentration data.18,20,21 The measured δ114/110Cd values of these reference materials are listed in Table 5. The δ114/110Cd values in these CRMs were obtained with a typical internal precision better than 0.050‰ (2 SE), which was consistent with the literature value5,7,14–33 within error.
To evaluate the accuracy of δ114/110Cd values obtained in this study, our results were compared with the published data. As shown in Fig. 4, the Cd isotope data show good agreement with the published datasets. Hence, these results demonstrate that the reproducibility and precision of the Cd isotope measurements achieved by the proposed method are satisfactory and fully meet the analytical requirements of environmental and geochemical research.
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