Modeling and forming the magnetic field of the heavy ion cyclotron
The heavy ion cyclotron was designed and constructed in the Dzhelepov Laboratory of Nuclear Problem, Joint Institute for Nuclear Research. Ions with A/Z~5 were accelerated up to the energy E=2.4 MeV/nucleon. The ECR source with an intensity of 3.5⋅10¹² ions/sec is used as an ion source. The extr...
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| Date: | 2004 |
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| Main Authors: | , , , , , |
| Format: | Article |
| Language: | English |
| Published: |
Національний науковий центр «Харківський фізико-технічний інститут» НАН України
2004
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| Series: | Вопросы атомной науки и техники |
| Subjects: | |
| Online Access: | https://nasplib.isofts.kiev.ua/handle/123456789/79366 |
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| Journal Title: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
| Cite this: | Modeling and forming the magnetic field of the heavy ion cyclotron / Yu.G. Alenitsky, A.F. Chesnov, S.A. Kostromin, L.M. Onischenko, E.V. Samsonov, N.L. Zaplatin // Вопросы атомной науки и техники. — 2004. — № 2. — С. 78-80. — Бібліогр.: 5 назв. — англ. |
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Digital Library of Periodicals of National Academy of Sciences of Ukraine| Summary: | The heavy ion cyclotron was designed and constructed in the Dzhelepov Laboratory of Nuclear Problem, Joint
Institute for Nuclear Research. Ions with A/Z~5 were accelerated up to the energy E=2.4 MeV/nucleon. The ECR
source with an intensity of 3.5⋅10¹² ions/sec is used as an ion source. The extracted beam of ~10¹¹ ions/sec is intended for the track membrane production. The magnetic field of this cyclotron is formed in the compact magnet with the pole diameter 1.6 m by means of four pairs of sector shims installed symmetrically up and down. The gaps are 100 mm, and 40 mm between the poles and shims, respectively. The proper dependence of the isochronous magnetic field on the radius is created, basically, by increasing the angular extension of sector shims inside the range α = 30º...41.8º. Power consumption of an electromagnet is 25 kW. |
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