Resonant recombination at ion storage rings: a conceptual alternative for isotope shift and hyperfine studies

C Brandau, C Kozhuharov, A Müller, D Bernhardt… - Hyperfine …, 2010 - Springer
C Brandau, C Kozhuharov, A Müller, D Bernhardt, F Bosch, D Boutin, FJ Currell
Hyperfine Interactions, 2010Springer
Sharp resonant structures in the cross section of the atomic electron-ion collision process of
dielectronic recombination are exploited to study isotope shifts and hyperfine interaction of
heavy highly-charged ions. This novel approach provides a conceptual alternative to
existing methods. In this contribution, we present a series of measurements, which we
performed at the heavy ion storage ring ESR of the GSI Helmholtzzentrum für
Schwerionenforschung, Darmstadt, Germany. In a first experiment the stable isotopes A …
Abstract
Sharp resonant structures in the cross section of the atomic electron-ion collision process of dielectronic recombination are exploited to study isotope shifts and hyperfine interaction of heavy highly-charged ions. This novel approach provides a conceptual alternative to existing methods. In this contribution, we present a series of measurements, which we performed at the heavy ion storage ring ESR of the GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany. In a first experiment the stable isotopes A = 142 and A = 150 of three-electron neodymium ANd57 +  were studied. Isotope shifts of dielectronic resonances associated with 2s − 2p j (j = 1/2, 3/2) transitions were extracted from the measured data. The evaluation of the energy shift was performed within a full QED framework and yielded a change in the mean-square charge radius of  fm2. At GSI, in addition to the investigation of stable isotopes unstable species can be artificially synthesized and studied. Radioisotopes produced in-flight from fragmentation of a 238U primary beam were injected into the ESR and were subsequently separated by their mass-to-charge ratio. This enabled us to perform first DR experiments with the exotic nuclei 237U89 +  (Z = 92 )and 234Pa88 +  (Z = 91).
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