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Performance of Ion Surfing Rf-carpets for High-Energy RI Beam Gas Catcher
Author(s) -
Fumiya Arai,
Y. Ito,
Ichiro Katayama,
P. Schury,
T. Sonoda,
M. Wada,
H. Wöllnik
Publication year - 2015
Publication title -
proceedings of the conference on advances in radioactive isotope science (aris2014)
Language(s) - English
Resource type - Conference proceedings
DOI - 10.7566/jpscp.6.030110
Subject(s) - ion , beam (structure) , ion beam , beam energy , radio frequency , materials science , electrical engineering , computer science , optoelectronics , nuclear engineering , physics , engineering , optics , quantum mechanics
High-energy radioactive isotopes have been used in ion trap-based precision experiments after being stopped in a large gas cell. The stopped ions of these isotopes can be extracted from the large gas cell as a low-energy ion beam. To transport and extract these ions quickly and efficiently, electric fields are required to guide them. In this respect, an rf-carpet (RFC) method utilizing a dc potential gradient is a standard technique. However, such a method is restricted to longer half-life isotopes because of the transport time owing to the upper limit on the dc gradient that can be supported before electric discharges occur in the large gas cell. To study short half-life isotopes, an RFC featuring faster transport is required. Recently, a hybrid technique wherein the dc gradient is replaced by a traveling potential wave was proposed, called ion surfing. Recently, we have demonstrated the transport and extraction of K ions using a circular RFC in 20 mbar of He gas pressure. However, in a practical gas cell, the gas pressure is higher by one order of magnitude. In this study, the transport and extraction of K and Cs ions with the ion surfing method were tested in high pressure He gas using a 100 mm cylinder electrode to create a push electric field Epush and a circular RFC of 80 mm diameter. In addition, we compared the effect of an RFC of a fine pitch with one of a rough pitch. The fine pitch RFC consists of 0.08 mm wide ring electrodes with 0.16 mm pitch and 0.32 mm diameter orifice, whereas the rough pitch RFC consists of 0.16 mm wide ring electrodes with 0.32 mm pitch and 0.64 mm diameter orifice.

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