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Application of capillary electrophoresis interfaced to double focusing sector field ICP-MS for nuclide abundance determination of lanthanides produced via spallation reactions in an irradiated tantalum targetPresented in part as poster No. 558 at the 1999 Federation of Analytical Chemistry and Spectroscopy Societies (FACSS) Conference, Vancouver, Canada, October 24–29, 1999.

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Application of capillary electrophoresis interfaced to double focusing sector field ICP-MS for nuclide abundance determination of lanthanides produced via spallation reactions in an irradiated tantalum targetPresented in part as poster No. 558 at the 1999 Federation of Analytical Chemistry and Spectroscopy Societies (FACSS) Conference, Vancouver, Canada, October 24–29, 1999.

Auteurs : Jason A. Day [États-Unis] ; Joseph A. Caruso [États-Unis] ; J. Sabine Becker [Allemagne] ; Hans-Joachim Dietze [Allemagne]

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RBID : ISTEX:A019964CF589DF157A495EA8B3C5DAA5A4015A03

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Abstract

An analytical procedure was developed using capillary electrophoresis (CE) coupled on-line to a double-focusing sector field inductively coupled plasma mass spectrometer (DF-ICP-MS) for the analysis of mixtures of lanthanide elements in aqueous samples with natural isotope abundances and in a sample taken from an irradiated tantalum target containing artificial nuclide abundances. A MicroMist AR30-1-F02 nebulizer with a Cinnabar small volume cyclonic spray chamber was used for ICP-MS sample introduction. The CE-ICP-MS interface featured a self-aspirating electrolyte make-up solution for electrical ground connection and control of nebulizer suction. The CE-ICP-MS method features fast run times and small sample sizes (≈35 nL injection volume). Detection limits for the most abundant lanthanide isotopes were 0.72 ppb to 3.9 ppb, an improvement of as much as one order of magnitude compared to a quadrupole ICP-MS system using a similar experimental arrangement. Abundances of the most abundant isotopes of lanthanides were found to be within 0.1–2% of table values for natural samples while isotopes present in smaller amounts were within 3–5% of table values. The method was applied to samples taken from a tantalum material which was exposed to a high energy proton beam for the production of neutrons via spallation reactions. A large fraction of the spallation products were lanthanides containing nuclide abundances unlike natural samples. Thus, a chemical separation step prior to ICP-MS detection was required to avoid isobaric interferences for the accurate determination of nuclide abundances in such samples. The results of the nuclide abundance determinations were compared to theoretical calculations.

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DOI: 10.1039/b002617o

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<title>Application of capillary electrophoresis interfaced to double focusing sector field ICP-MS for nuclide abundance determination of lanthanides produced via spallation reactions in an irradiated tantalum targetPresented in part as poster No. 558 at the 1999 Federation of Analytical Chemistry and Spectroscopy Societies (FACSS) Conference, Vancouver, Canada, October 24–29, 1999.</title>
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<term>Absorbance detection</term>
<term>Abundant isotopes</term>
<term>Accurate determination</term>
<term>Anal</term>
<term>Background signals</term>
<term>Capillary</term>
<term>Capillary electrophoresis</term>
<term>Capillary position</term>
<term>Chemical separation step</term>
<term>Chemische analysen</term>
<term>Copper wire</term>
<term>Deionized water</term>
<term>Detection limits</term>
<term>Dysprosium isotopes</term>
<term>Electrolyte</term>
<term>Electrolyte solution</term>
<term>Experimental values</term>
<term>Hiba</term>
<term>High energy proton beam</term>
<term>Icpms detection</term>
<term>Injection volume</term>
<term>Interface</term>
<term>Isobaric interferences</term>
<term>Isotope</term>
<term>Lanthanide</term>
<term>Lanthanide elements</term>
<term>Lower abundance isotopes</term>
<term>Micromist nebulizer</term>
<term>Migration times</term>
<term>Nancial support</term>
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<term>Natural isotope abundances</term>
<term>Natural isotope ratios</term>
<term>Natural samples</term>
<term>Nebulizer</term>
<term>Nebulizer suction</term>
<term>Nuclide</term>
<term>Nuclide abundance</term>
<term>Nuclide abundances</term>
<term>Nuclides</term>
<term>Peak area</term>
<term>Peak areas</term>
<term>Peak data</term>
<term>Peak shapes</term>
<term>Peak widths</term>
<term>Peek</term>
<term>Peek sleeve</term>
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<term>Polyatomic interferences</term>
<term>Relative abundances</term>
<term>Separation conditions</term>
<term>Small chips</term>
<term>Small sample amounts</term>
<term>Spallation</term>
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<term>Spallation reactions</term>
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<term>Spray chamber</term>
<term>Such samples</term>
<term>Suction</term>
<term>Sutton</term>
<term>Table values</term>
<term>Tantalum</term>
<term>Tantalum material</term>
<term>Tantalum target</term>
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<term>Tantalum target sample</term>
<term>Tantalum target samples</term>
<term>Theoretical calculations</term>
<term>Theoretical predictions</term>
<term>Volume cyclonic spray chamber</term>
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<term>Background signals</term>
<term>Capillary</term>
<term>Capillary electrophoresis</term>
<term>Capillary position</term>
<term>Chemical separation step</term>
<term>Chemische analysen</term>
<term>Copper wire</term>
<term>Deionized water</term>
<term>Detection limits</term>
<term>Dysprosium isotopes</term>
<term>Electrolyte</term>
<term>Electrolyte solution</term>
<term>Experimental values</term>
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<term>High energy proton beam</term>
<term>Icpms detection</term>
<term>Injection volume</term>
<term>Interface</term>
<term>Isobaric interferences</term>
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<term>Lanthanide</term>
<term>Lanthanide elements</term>
<term>Lower abundance isotopes</term>
<term>Micromist nebulizer</term>
<term>Migration times</term>
<term>Nancial support</term>
<term>Natural abundances</term>
<term>Natural isotope abundances</term>
<term>Natural isotope ratios</term>
<term>Natural samples</term>
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<term>Nebulizer suction</term>
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<term>Nuclide abundance</term>
<term>Nuclide abundances</term>
<term>Nuclides</term>
<term>Peak area</term>
<term>Peak areas</term>
<term>Peak data</term>
<term>Peak shapes</term>
<term>Peak widths</term>
<term>Peek</term>
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<term>Polyatomic interferences</term>
<term>Relative abundances</term>
<term>Separation conditions</term>
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<div type="abstract">An analytical procedure was developed using capillary electrophoresis (CE) coupled on-line to a double-focusing sector field inductively coupled plasma mass spectrometer (DF-ICP-MS) for the analysis of mixtures of lanthanide elements in aqueous samples with natural isotope abundances and in a sample taken from an irradiated tantalum target containing artificial nuclide abundances. A MicroMist AR30-1-F02 nebulizer with a Cinnabar small volume cyclonic spray chamber was used for ICP-MS sample introduction. The CE-ICP-MS interface featured a self-aspirating electrolyte make-up solution for electrical ground connection and control of nebulizer suction. The CE-ICP-MS method features fast run times and small sample sizes (≈35 nL injection volume). Detection limits for the most abundant lanthanide isotopes were 0.72 ppb to 3.9 ppb, an improvement of as much as one order of magnitude compared to a quadrupole ICP-MS system using a similar experimental arrangement. Abundances of the most abundant isotopes of lanthanides were found to be within 0.1–2% of table values for natural samples while isotopes present in smaller amounts were within 3–5% of table values. The method was applied to samples taken from a tantalum material which was exposed to a high energy proton beam for the production of neutrons via spallation reactions. A large fraction of the spallation products were lanthanides containing nuclide abundances unlike natural samples. Thus, a chemical separation step prior to ICP-MS detection was required to avoid isobaric interferences for the accurate determination of nuclide abundances in such samples. The results of the nuclide abundance determinations were compared to theoretical calculations.</div>
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