J. Ullrich

Major role of multielectronic K-L inter-shell resonant recombination processes in Li- to O-like ions of Ar, Fe, and Kr

C. Beilmann [1], Z. Harman [1,2], P. H. Mokler [1], S. Bernitt [1], C. H. Keitel [1], J. Ullrich [1], J. R. Crespo López-Urrutia

Abstract

Dielectronic and higher-order resonant electron recombination processes including a K-shell excitation were systematically measured at high resolution in electron beam ion traps. Storing highly charged Ar, Fe, and Kr ions, the dependence on atomic number Z of the contribution of these processes to the total recombination cross section was studied and compared with theoretical calculations. Large higher-order resonant recombination contributions are found, especially for systems with 10<Z<36. In some cases, they even surpass the strength of the dielectronic channel, which was hitherto presumed to be always the dominant one. These findings have consequences for the modeling of high-temperatur plasmas. Features attributed to inter-shell quadruelectronic recombination were also observed. The experimental data obtained for the He-like to O-like isoelectronic sequences compare well with the results of advanced relativistic distorted-wave calculations employing multiconfiguration Dirac-Fock bound state wave functions that include threefold and fourfold excitations.

Decay rate measurement of the first vibrationally excited state of MgH$^+$ in a cryogenic Paul trap

O. O. Versolato [1], M. Schwarz [1], A. K. Hansen [2], A. D. Gingell [2], A. Windberger [1,3], Å\udc81. KÅ‚osowski, J. Ullrich [1,4], F. Jensen [5,1], J. R. Crespo López-Urrutia, M. Drewsen [2]

Abstract

We present a method to measure the decay rate of the first excited vibrational state of simple polar molecular ions being part of a Coulomb crystal in a cryogenic linear Paul trap. Specifically, we have monitored the decay of the $|ν$=$1,J$=$1 \rangle_X$ towards the $|ν$=$0,J$=$0 \rangle_X$ level in MgH$^+$ by saturated laser excitation of the $|ν$=$0,J$=$2 \rangle_X$-$|ν$=$1,J$=$1 \rangle_X$ transition followed by state selective resonance enhanced two-photon dissociation out of the $|ν$=$0,J$=$2 \rangle_X$ level. The technique enables the determination of decay rates, and thus absorption strengths, with an accuracy at the few percent level.

First Use of High Charge States for Mass Measurements of Short-lived Nuclides in a Penning Trap

S. Ettenauer [1,2], M. C. Simon [1], A. T. Gallant [1,2], T. Brunner [1,3], U. Chowdhury [1,4], V. V. Simon [1,5,6], M. Brodeur [1,2,7], A. Chaudhuri [1], E. Mané, C. Andreoiu [8], G. Audi [9,5], J. R. Crespo López-Urrutia, P. Delheij [1], G. Gwinner [4], A. Lapierre [1,7], D. Lunney [1,9], M. R. Pearson [1], R. Ringle [7], J. Ullrich [5], J. Dilling [1,2]

Abstract

Penning trap mass measurements of short-lived nuclides have been performed for the first time with highly-charged ions (HCI), using the TITAN facility at TRIUMF. Compared to singly-charged ions, this provides an improvement in experimental precision that scales with the charge state q. Neutron-deficient Rb-isotopes have been charge bred in an electron beam ion trap to q = 8 - 12+ prior to injection into the Penning trap. In combination with the Ramsey excitation scheme, this unique setup creating low energy, highly-charged ions at a radioactive beam facility opens the door to unrivalled precision with gains of 1-2 orders of magnitude. The method is particularly suited for short-lived nuclides such as the superallowed β emitter 74Rb (T1/2 = 65 ms). The determination of its atomic mass and an improved QEC-value are presented.

A novel method for unambiguous ion identification in mixed ion beams extracted from an EBIT

W. Meissl [1], M. C. Simon [1,2], J. R. Crespo Lopez-Urrutia, H. Tawara [2], J. Ullrich [2], HP. Winter [1], F. Aumayr [1]

Abstract

A novel technique to identify small fluxes of mixed highly charged ion beams extracted from an Electron Beam Ion Trap (EBIT) is presented and practically demonstrated. The method exploits projectile charge state dependent potential emission of electrons as induced by ion impact on a metal surface to separate ions with identical or very similar mass-to-charge ratio.