Paper | Title | Page |
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MOP1WA02 |
IMP Heavy Ion Synchrotron | |
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This talks is about IMP heavy ion synchrotron. | ||
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Slides MOP1WA02 [8.382 MB] | |
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TUP2WA04 | Dynamic Vacuum Simulation for the BRing | 186 |
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Funding: Youth Innovation Promotion Association of Chinese Academy of Sciences 2016364, National Natural Science Foundation of China (Project No. 11675235). Large dynamic vacuum pressure rises of orders of magnitude which caused by the lost heavy ions can seriously limit the ion intensity and beam lifetime of the heavy ion accelerator, especially for the machine that operate the intermediate charge state heavy ion. The High Intensity heavy ion Accelerator Facility (HIAF) which will be built by the IMP will accumulate the intermediate charge state ion 238U35+ to intensity 2*1011 ppp to different terminals. In order to control the dynamic vacuum effects induced by the lose beams and design the collimation system for the BRing of the HIAF, a newly developed simulation program (ColBeam) and GSI's simulation code StrahlSim are both conducted and the dynamic vacuum simulation result is calculated by the StrahlSim. According to the simulation result, 3*1011 ppp particles is the up limit beam intensity can be extracted for the current BRing vacuum system design. Higher beam intensity can be reach to 5*1011 ppp when the NEG coating technology must be implemented for the dipole and quadrupole chamber. HIAF, Collimation, Dynamic vacuum |
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Slides TUP2WA04 [9.947 MB] | |
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-HB2018-TUP2WA04 | |
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WEP2PO024 | Resonance Stop-bands Compensation at Booster Ring of HIAF | 315 |
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Booster Ring (BRing) of the new approved High Intensity heavy-ion Accelerator Facility (HIAF) in China is designed to stack 0.3-1.0·1011 number of 238U35+ ions by painting injection and deliver over such intensity beam in extraction. However, depressed tune spread caused by space charge effect crosses the low-order resonance stop-bands after bunching the storage beam. To keep a low beam loss during crossing, stop-band compensation scheme is proposed covering the whole process of RF capture and early acceleration. | ||
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Poster WEP2PO024 [1.218 MB] | |
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-HB2018-WEP2PO024 | |
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