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Physical Review Letters

Observation of the metastable negative argon ion Ar−

Young K. Bae, James R. Peterson, A. S. Schlachter, J. Warren Stearns

Published Feb 25, 1985• 22 citations
Publisher

Abstract

The predicted metastable $^{4}\mathrm{S}_{3/2}^{\mathrm{e}}$ ${\mathrm{Ar}}^{\mathrm{\ensuremath{-}}}$ ion has been observed for the first time. It was produced from an ${\mathrm{Ar}}^{+}$ beam by two-step electron capture in Cs vapor. Decay-rate measurements favor the existence of only one state with a lifetime of 350\ifmmode\pm\else\textpm\fi{}150 ns.

DOI
10.1103/physrevlett.54.789

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The predicted metastable 4S3/2e^{4}\mathrm{S}_{3/2}^{\mathrm{e}}4S3/2e​ Ar\ensuremath−{\mathrm{Ar}}^{\mathrm{\ensuremath{-}}}Ar\ensuremath− ion has been observed for the first time. It was produced from an Ar+{\mathrm{Ar}}^{+}Ar+ beam by two-step electron capture in Cs vapor. Decay-rate measurements favor the existence of only one state with a lifetime of 350\ifmmode\pm\else\textpm\fi{}150 ns.
Long-lived metastable ${\mathrm{He}}_{2}^{\ensuremath{-}}$ negative ions have been observed for the first time. They were produced from He2+{\mathrm{He}}_{2}^{+}He2+​ by two-step electron capture in a Cs vapor target. The apparent autodetachment decay rates have been measured at several delay times after formation, and indicate the presence of more than one state, with the lifetime of the major component exceeding 100 \ensuremath{\mu}s. The most likely configurations are ${^{4}\ensuremath{\Sigma}_{g}}^{+}$ and/or $^{4}\ensuremath{\Pi}_{g}$ states bound below ${\mathrm{He}}_{2}({^{3}\ensuremath{\Sigma}_{g}}^{+})$.
The natural lifetime of the metastable 4d2D5∕24d\phantom{\rule{0.2em}{0ex}}^{2}D_{5∕2}4d2D5∕2​ state in 88Sr+^{88}\mathrm{Sr}^{+}88Sr+ has been measured using a single laser-cooled, trapped ion. The ion was prepared in the 4d2D5∕24d\phantom{\rule{0.2em}{0ex}}^{2}D_{5∕2}4d2D5∕2​ state by laser excitation of the $5s\phantom{\rule{0.2em}{0ex}}^{2}S_{1∕2}\ensuremath{-}4d\phantom{\rule{0.2em}{0ex}}^{2}D_{5∕2}$ quadrupole transition at 674 nm. The decay time was measured by using Dehmelt's electron shelving method to monitor the ion's electronic state. Two separate investigations were conducted under slightly different experimental conditions. 160 000 decay times from the 4d2D5∕24d\phantom{\rule{0.2em}{0ex}}^{2}D_{5∕2}4d2D5∕2​ state were observed in total, and two different methods for determining the statistical value of the measured lifetime have been compared. Systematic effects have also been estimated, and including these effects yields a value of $\ensuremath{\tau}=390.8(1.6)\phantom{\rule{0.3em}{0ex}}\mathrm{ms}$ ($1\ensuremath{\sigma}$ uncertainty) for the natural lifetime.
This paper presents a combined experimental and theoretical investigation of the binding energy of the metastable ${\mathrm{Ar}}^{\ensuremath{-}}{(3p}^{5}4s4p{}^{4}{S}_{3/2}^{e})$ ion. Utilizing the laser-photodetachment threshold technique combined with state-selective detection of neutral atoms by resonant ionization spectroscopy, we find a binding energy of $32.5\ifmmode\pm\else\textpm\fi{}1.0$ meV with respect to the 3p54s3P2o{3p}^{5}4s{}^{3}{P}_{2}^{o}3p54s3P2o​ state of neutral argon. Our calculations, based on many-body perturbation theory, yield a binding energy of 24.9 meV. As a test of the present computational method, we also include the results of a comparative study of ${\mathrm{Ca}}^{\ensuremath{-}}$.
The lifetime of the metastable autodetaching 1s2s2p 4^{4}4P5/2{\mathit{P}}_{5/2}P5/2​ level of the $^{4}\mathrm{He}^{\mathrm{\ensuremath{-}}}$ ion has been measured by a time-of-flight technique to be 350\ifmmode\pm\else\textpm\fi{}15 \ensuremath{\mu}s using a heavy-ion storage ring. Blackbody-induced photodetachment of this weakly bound level is shown to influence the decay rate by nearly 20%, an effect not discussed previously. The magnetic-field-induced mixing effects provide additional information about the lifetime of the close-lying 4^{4}4P3/2{\mathit{P}}_{3/2}P3/2​ level, yielding \ensuremath{\tau}(4{(}^{4}(4P3/2{\mathit{P}}_{3/2}P3/2​)=12\ifmmode\pm\else\textpm\fi{}2 \ensuremath{\mu}s. The observed lifetimes are consistent with previous experimental values, but the accuracy of the 4^{4}4P5/2{\mathit{P}}_{5/2}P5/2​ lifetime is improved by a factor of 6, allowing a detailed test of theoretical predictions to be performed. The 4^{4}4P5/2{\mathit{P}}_{5/2}P5/2​ lifetime is significantly shorter than most recent advanced theoretical results, but in agreement with a multiconfiguration Hartree-Fock approach accurately describing the initial bound 4^{4}4P5/2{\mathit{P}}_{5/2}P5/2​ and the final continuum 2^{2}2F5/2{\mathit{F}}_{5/2}F5/2​ states.
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