Paper |
Title |
Page |
THPAL113 |
The Design of 1 MeV Proton LINAC Operating in CW |
3905 |
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- N.V. Avreline
TRIUMF, Vancouver, Canada
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Experimental results and computer simulations of electrodynamic and thermodynamic characteristics are presented for an accelerating structure that is excited in the TM010 mode and that has the accelerating channel of URAN-1M located in the diametric plane. The idea of using this structure in the particle accelerator URAN-1M, located at the Baikov Institute of Metallurgy and Materials Science, with the goal of increasing the average beam current is explored.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-IPAC2018-THPAL113
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THPAL114 |
The Analytical Model of the Helical Accelerating Structure of Linac with Helix Outside of the Vacuum Chamber |
3908 |
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- N.V. Avreline
TRIUMF, Vancouver, Canada
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An analytical model of the helical RF resonator for the single charged 250 keV nitrogen ion implanter operating in CW was developed. The analytical model allowed to determine the geometry of the accelerating structure and to construct CST Microwave Studio and ANSYS HFSS models based on this analytical model. Results obtained from the analytical model and simulations were within 5% of each other. The experimental investigation of the accelerating section confirmed that the models are correct. The accelerating section was tuned and verified for the right accelerating field distribution and operating frequency. Finally, the section was successfully tested in 2 kW CW RF power.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-IPAC2018-THPAL114
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THPAL115 |
The Design of 1.1 MW RF Dummy Load for the RF System of 520 MeV Cyclotron |
3911 |
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- N.V. Avreline, Y. Bylinskii, B. Jakovljevic, Y. Ma, V. Zvyagintsev
TRIUMF, Vancouver, Canada
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The RF System of 520-MeV Cyclotron is operating at 23 MHz with 1 MW CW RF power. The RF dummy load is required to troubleshoot and tune the RF amplifier. The RF system is being constantly improved and the future goal is to increase cyclotron's beam current up to 400 μA, which requires increasing the RF amplifier's power. As a part of this goal, a new RF dummy load was designed.
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|
DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-IPAC2018-THPAL115
|
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