Paper |
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MOA2CIO01 |
HIRFL-CSR Facility Status and Development |
37 |
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- Y.J. Yuan, X.H. Cai, D.Q. Gao, Y. He, L.Z. Ma, X. Ma, R.S. Mao, Y.W. Su, X.L. Tu, J.W. Xia, H.S. Xu, Z. Xu, J.C. Yang, X.D. Yang, X.T. Yang, Y.P. Yang, W. Zhang, H.W. Zhao
IMP, Lanzhou, People's Republic of China
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The HIRFL-CSR facility come into operation by the end of 2007. During operation in recent years, CSR supplied beam for experiments at several terminals and inside both CSRm and CSRe rings. The experiments covers high resolution mass measurement, cancer therapy research, neutron wall, atomic physics using electron target and internal gas target, using injection beam mainly from the SFC of cyclotron injector. New methods and further developments are required to improve the performance of CSR system including multi-gradients measurement method for beam spot commissioning and beam transfer, nonlinear effect correction and stabilization of isochronous mode of CSRe. For suppling of heverier ion beam with proper ernergy, the cyclotron complex should be enhanced and new injector is proposed to replace SFC as injector of SSC.
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Slides MOA2CIO01 [3.766 MB]
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MOPCP105 |
Research on Acceptance of SSC |
260 |
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- X.N. Li, Y. He, Y.J. Yuan
IMP, Lanzhou, People's Republic of China
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The injection, acceleration and extraction of SSC (Separate Sector Cyclotron) is analyzed and simulated to get the transverse and longitudinal acceptance, using two typical ions 238U36+ and 70Zn10+ with energy 9.7 MeV/u and 5.62 MeV/u respectively. In order to study the actual acceptance of SSC, the isochronous magnetic field model in coincidence with the real one is established by Kr-Kb and Lagrange methods based on the actual measurement. The transverse and longitudinal acceptance is calculated under the above isochronous magnetic field model. From the simulation results, one of the major reason of low efficiency and acceptance of SSC is the defaults in the design of MSI3. The simulation results show that the actual efficiency and acceptance of SSC can be improved by redesign the curvature of MSI3 or shim in MSI3 to change the distribution of inner magnetic field.
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