2011
DOI: 10.1103/physreva.83.012711
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Dielectronic recombination of xenonlike tungsten ions

Abstract: Dielectronic recombination (DR) of xenonlike W20+ forming W19+ has been studied experimentally at a heavy-ion storage-ring. A merged-beams method has been employed for obtaining absolute rate coefficients for electron-ion recombination in the collision energy range 0-140 eV. The measured rate coefficient is dominated by strong DR resonances even at the lowest experimental energies. At plasma temperatures where the fractional abundance of W20+ is expected to peak in a fusion plasma, the experimentally derived p… Show more

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Cited by 92 publications
(164 citation statements)
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“…Experiment shows that the recombination rates at low (∼ 1 eV) electron energies in these ions exceed the direct RR rates by two orders of magnitude or more. At the same time the measured rates do not show the sharp resonance structure normally associated with DR [14,19,36]. The MBQC statistical theory quantitatively explains the discrepancy as being due to a very dense spectrum of compound resonances: multiply excited, strongly mixed, chaotic many-electron eigenstates.…”
Section: Theorymentioning
confidence: 77%
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“…Experiment shows that the recombination rates at low (∼ 1 eV) electron energies in these ions exceed the direct RR rates by two orders of magnitude or more. At the same time the measured rates do not show the sharp resonance structure normally associated with DR [14,19,36]. The MBQC statistical theory quantitatively explains the discrepancy as being due to a very dense spectrum of compound resonances: multiply excited, strongly mixed, chaotic many-electron eigenstates.…”
Section: Theorymentioning
confidence: 77%
“…In the future our levelresolved statistical theory can also be applied to other processes where chaotic mixing plays an important role, such as photo-and electron-impact ionization and scattering processes in highly charged ions [20]. [14] (black) and the theoretical results of this paper (red). The latter is obtained by multiplying our capture rate (dot-dashed line) with our extracted fluorescence yield (18).…”
Section: Discussionmentioning
confidence: 99%
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“…The 2s 2p 3 P 0 state is the lowest excited state, and for isotopes with a nonzero nuclear spin, the J = 0 → 0 transition channel * jon.grumer@teorfys.lu.se opens up due to mixing of the hyperfine levels, leading to a so-called hyperfine-induced transition (HIT). Such a shortening of lifetimes of metastable states owing to hyperfine interaction is referred to as hyperfine quenching and has been investigated for Be-like ions both theoretically [15][16][17][18][19][20] and experimentally [21,22]. For isotopes with zero nuclear spin, on the other hand, a one-photon transition to the ground state 2s 2 1 S 0 is strictly forbidden in a field-free region, and the lowest-order decay channel is a very slow E1M1 two-photon process.…”
Section: Introductionmentioning
confidence: 99%