2020
DOI: 10.1016/j.nimb.2019.05.016
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A gas-jet apparatus for high-resolution laser spectroscopy on the heaviest elements at SHIP

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Cited by 19 publications
(38 citation statements)
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“…With the short cycle, it was possible to detect 154 Yb from resonant laser ionization for the first time. The limited resolution in the gas cell [27] did not allow resolving the hyperfine structure of three expected hyperfine components in 155 Yb with a nuclear spin of I = 7/2. In addition, the expected isotope shift of around 1 GHz [29][30][31][32] is much smaller compared to the spectral linewidth of the FES laser of approximately 6 GHz and has therefore not been properly determined with the available statistics.…”
Section: Results With the Short Radris Cycle Implementationmentioning
confidence: 99%
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“…With the short cycle, it was possible to detect 154 Yb from resonant laser ionization for the first time. The limited resolution in the gas cell [27] did not allow resolving the hyperfine structure of three expected hyperfine components in 155 Yb with a nuclear spin of I = 7/2. In addition, the expected isotope shift of around 1 GHz [29][30][31][32] is much smaller compared to the spectral linewidth of the FES laser of approximately 6 GHz and has therefore not been properly determined with the available statistics.…”
Section: Results With the Short Radris Cycle Implementationmentioning
confidence: 99%
“…Due to the limited mobility [6,26] of the Yb ions in the argon buffer gas, the ions reach the detector with a certain delay. The stopping distribution of the recoils in the gas cell [27] in addition to diffusion processes lead to an increased width of the distribution of the ions' arrival time at the detector. To determine the time required for the ions to reach the detector, one has to solve the differential equation describing the increasing number of 154 Yb ions on the detector after every accelerator beam pulse with respect to their successive decay as…”
Section: Short Radris Cycle Developmentmentioning
confidence: 99%
“…This new technique enabled a detailed characterization of gas jets created by different nozzle geometries [175]. Dedicated apparatuses are developed to employ laser spectroscopy in a supersonic gas jet at the in-flight separator S 3 at GANIL [173,129], the Mass Analysing Recoil Apparatus (MARA) separator at Jyväskylä University [176,177] and in a modified version using ionguiding electric fields and neutralization on filaments at the Separator for Heavy-Ion reaction Products (SHIP) of the GSI [178].…”
Section: Laser Ionization In a Gas Jetmentioning
confidence: 99%
“…Due to the pressure and temperature conditions in the gas cell, the spectral resolution is limited to about 3 GHz. This is often insufficient to resolve all individual hyperfine components of the studied optical transition, as, e.g., in the case of 253 No [10]. Additionally, species with half-lives of less than approximately one second are inaccessible to the RADRIS technique due to decay losses during recoil ion collection.…”
Section: Introductionmentioning
confidence: 99%
“…Additionally, species with half-lives of less than approximately one second are inaccessible to the RADRIS technique due to decay losses during recoil ion collection. To overcome both of these limitations, JetRIS has been constructed for high-resolution resonance ionization spectroscopy in a hypersonic gas-jet [10]. JetRIS combines the high resolution of the in-gas-jet laser spectroscopy technique developed at KU Leuven [11][12][13] with the sensitivity of the ion collection and neutral desorption from a heated filament used in the RADRIS technique [14,15].…”
Section: Introductionmentioning
confidence: 99%