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Performance of a Resonant Schottky Pick-Up for the Rare-RI Ring Project
Author(s) -
Fumi Suzaki,
J. Zenihiro,
Yasushi Abe,
Akira Ozawa,
Takeshi Suzuki,
Т. Уесака,
M. Wakasugi,
Kazunari Yamada,
Takayuki Yamaguchi
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.6.030119
Subject(s) - ring (chemistry) , schottky diode , materials science , optoelectronics , electrical engineering , physics , computer science , engineering , chemistry , organic chemistry , diode
Construction of a new storage ring called “Rare-RI Ring” was started in 2012 at RIBF. This project aims at precise isochronous mass measurements for extremely neutron-rich exotic nuclei in the r-process nucleosynthesis. To precisely tune the ion-optical condition to be isochronous, the resonant Schottky noise pick-up technique will be employed. We performed an off-line test of the resonant Schottky pick-up. Figure 1 shows the resonant Schottky pick-up that will be installed in the Rare-RI Ring. It consists of a pillbox-type resonant cavity electrically isolated from the beam pipe by a ceramic tube. A schematic view of the pick-up is shown in Fig. 2(a): a chamber shown in blue is the beam pipe and the shaded cylinder surrounding the beam pipe is the cavity equipped with two ports (yellow). The ports are movable plunger pistons that can adjust the resonance frequency (fres) of the eigenmode. Fig. 2(b) shows the cross-sectional view of the cavity, and the detailed structure of the gap can be seen at the center. The cavity itself is filled with air and has the shape of a pillbox with an outer diameter of 750 mm and length of 200 mm. The inner diameter is 320 mm. The lower flanges ( see Fig. 1 ) are prepared for feedthroughs to take out signals from a loop coil that magnetically couples to the cavity field induced by the beam. Using a network analyzer, we measured the basic quantities characterizing the resonant cavity: the resonance frequency, the shunt impedance Rsh, and the unloaded Q factor Q0. To measure Rsh, the perturbation method was adopted. From the measurements, fres = 171.54(±0.44) MHz, Rsh = 169 kΩ, and Q0 = 1884 were obtained. For tuning the isochronous field settings, the proposed pick-up is required to have an excellent singleion sensitivity. By using the results of the off-line test, the output signal power corresponding to a single ion with charge q at resonance is estimated to be P = q × 2.8 × 10−21 W , and the power of thermal noise Pnoise is 7.1 × 10−19 W. For q ≥ 16, the signal power exceeds the noise floor, and the signal from the beam can be detected by the present Schottky pickup. Therefore, the performance is sufficient for precise tuning of isochronus field settings of the Rare-RI Ring. The resonant Schottky pick-up will be soon installed into the Rare-RI Ring. Detailed results of the off-line test and online beam performance test will be reported

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