Improvement of the RF cavity for the SKKUCY-10 cyclotron

The SKKUCY-10 cyclotron based on 83.2 MHz, 40 kV half-wave RF cavity was developed at Sungkyunkwan University for the production of medical radioisotopes. The resonant frequency f RF of the cyclotron and the RF coupling coefficient β c of the RF cavity system were measured at various vacuum, and tem...

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Published inJournal of the Korean Physical Society Vol. 79; no. 9; pp. 857 - 863
Main Authors Lee, Jongchul, Ghergherehchi, Mitra, Gad, Khaled M. M., Ha, Donghyup, Namgoong, Ho, Lee, Seunghyun, Song, Ho Seung, Karatas, Berat Can, Chai, Jong-Seo
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LanguageEnglish
Published Seoul The Korean Physical Society 01.11.2021
Springer Nature B.V
한국물리학회
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Abstract The SKKUCY-10 cyclotron based on 83.2 MHz, 40 kV half-wave RF cavity was developed at Sungkyunkwan University for the production of medical radioisotopes. The resonant frequency f RF of the cyclotron and the RF coupling coefficient β c of the RF cavity system were measured at various vacuum, and temperature conditions. The normalized multi-pacting intensities at four positions in the power coupler were analyzed to predict the multi-pacting power. Differences, Δ f RF and Δ β c , caused by the vacuum, and temperature conditions were modified based on the coupler and tuner gap distances. During the RF conditioning, a constant 15 kW pulse mode and a variable 1 to 15 kW continuous wave mode were employed. The values of the reflection coefficient Γ and β c were 1.2% and 0.8, respectively, when the cavity dissipation power was 12.4 kW at 83.2 MHz. Good agreement between the simulation and experimental data was obtained.
AbstractList The SKKUCY-10 cyclotron based on 83.2 MHz, 40 kV half-wave RF cavity was developed at Sungkyunkwan University for the production of medical radioisotopes. The resonant frequency fRF of the cyclotron and the RF coupling coefficient βc of the RF cavity system were measured at various vacuum, and temperature conditions. The normalized multi-pacting intensities at four positions in the power coupler were analyzed to predict the multi-pacting power. Differences, ΔfRF and Δβc , caused by the vacuum, and temperature conditions were modified based on the coupler and tuner gap distances. During the RF conditioning, a constant 15 kW pulse mode and a variable 1 to 15 kW continuous wave mode were employed. The values of the reflection coefficient Γ and βc were 1.2% and 0.8, respectively, when the cavity dissipation power was 12.4 kW at 83.2 MHz. Good agreement between the simulation and experimental data was obtained. KCI Citation Count: 0
The SKKUCY-10 cyclotron based on 83.2 MHz, 40 kV half-wave RF cavity was developed at Sungkyunkwan University for the production of medical radioisotopes. The resonant frequency f RF of the cyclotron and the RF coupling coefficient β c of the RF cavity system were measured at various vacuum, and temperature conditions. The normalized multi-pacting intensities at four positions in the power coupler were analyzed to predict the multi-pacting power. Differences, Δ f RF and Δ β c , caused by the vacuum, and temperature conditions were modified based on the coupler and tuner gap distances. During the RF conditioning, a constant 15 kW pulse mode and a variable 1 to 15 kW continuous wave mode were employed. The values of the reflection coefficient Γ and β c were 1.2% and 0.8, respectively, when the cavity dissipation power was 12.4 kW at 83.2 MHz. Good agreement between the simulation and experimental data was obtained.
The SKKUCY-10 cyclotron based on 83.2 MHz, 40 kV half-wave RF cavity was developed at Sungkyunkwan University for the production of medical radioisotopes. The resonant frequency fRF of the cyclotron and the RF coupling coefficient βc of the RF cavity system were measured at various vacuum, and temperature conditions. The normalized multi-pacting intensities at four positions in the power coupler were analyzed to predict the multi-pacting power. Differences, ΔfRF and Δβc, caused by the vacuum, and temperature conditions were modified based on the coupler and tuner gap distances. During the RF conditioning, a constant 15 kW pulse mode and a variable 1 to 15 kW continuous wave mode were employed. The values of the reflection coefficient Γ and βc were 1.2% and 0.8, respectively, when the cavity dissipation power was 12.4 kW at 83.2 MHz. Good agreement between the simulation and experimental data was obtained.
Author Namgoong, Ho
Gad, Khaled M. M.
Karatas, Berat Can
Lee, Jongchul
Ghergherehchi, Mitra
Lee, Seunghyun
Ha, Donghyup
Chai, Jong-Seo
Song, Ho Seung
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Keywords RF cavity
Cyclotron
RF conditioning
Coupling coefficient
Resonant frequency
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Snippet The SKKUCY-10 cyclotron based on 83.2 MHz, 40 kV half-wave RF cavity was developed at Sungkyunkwan University for the production of medical radioisotopes. The...
The SKKUCY-10 cyclotron based on 83.2 MHz, 40 kV half-wave RF cavity was developed at Sungkyunkwan University for the production of medical radioisotopes. The...
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SubjectTerms Continuous radiation
Couplers
Coupling coefficients
Mathematical and Computational Physics
Original Paper
Particle and Nuclear Physics
Physics
Physics and Astronomy
Radioisotopes
Reflectance
Resonant frequencies
Theoretical
물리학
Title Improvement of the RF cavity for the SKKUCY-10 cyclotron
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