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Effect of impact energy on SIMS U–Pb zircon geochronology
Author(s) -
Magee Charles,
Ferris Jim,
Magee Charles
Publication year - 2014
Publication title -
surface and interface analysis
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.52
H-Index - 90
eISSN - 1096-9918
pISSN - 0142-2421
DOI - 10.1002/sia.5629
Subject(s) - zircon , microprobe , analytical chemistry (journal) , geochronology , fractionation , secondary ion mass spectrometry , sputtering , ion , chemistry , yield (engineering) , materials science , geology , mineralogy , geochemistry , thin film , environmental chemistry , nanotechnology , metallurgy , organic chemistry
Secondary ion mass spectrometry (SIMS) measurements of Pb isotopes and U–Pb elemental ratios in natural minerals are one of the most important methods of measuring geologic time on the million to billion year timescale. Precise and accurate geochronology requires accurate correction of elemental U and Pb fractionation in the SIMS process. The calibration schemes used to correct for this fractionation have been in use since the 1990s. However, the mechanism by which they work remains poorly understood. The independence of primary ion impact energy from the secondary voltage in the sensitive high‐resolution ion microprobe (SHRIMP) is used to examine the ionization efficiency of Pb + in zircon over a range of impact energies from 3.7 kV to 15.7 kV. A plateau of around 34 cps/nA O 2 − /ppm 206 Pb is observed between 5.7 and 10.7‐kV impact energy. In contrast, useful yield increases steadily as impact energy is decreased. The use of a primary beam made of 18 O 2 − ions allows the 18 O implanted by the primary beam to be differentiated from the 16 O in the natural silicate matrix. The oxygen isotopic results, with larger 18 O/ 16 O ratios at lower energies, suggest that enhanced oxygen activity at the sputtering surface may be due to progressively lower sputtering efficiency at lower energies. This would increase the Pb + yield from the sample even as the ion yield per nA of primary beam remains constant, as a nA of molecular oxygen at 5 kV or less sputters a smaller sample volume than at higher energies. The useful yield for Pb increases from 1% to 3% as the primary energy drops. Copyright © 2014 John Wiley & Sons, Ltd.