Dynamic vacuum simulation for the Booster Ring in the high-intensity heavy ion accelerator facility

被引：3

作者：

Li, Peng ^{[1
]}

Bozyk, Lars ^{[2
]}

Dong, Zhiqiang ^{[1
]}

Spiller, Peter ^{[2
]}

Li, Min ^{[1
]}

Yang, Jiancheng ^{[1
]}

Yuan, Youjin ^{[1
]}

Luo, Cheng ^{[1
]}

Xie, Wenjun ^{[1
]}

Zhen, Wenheng ^{[1
]}

机构：

[1] Chinese Acad Sci, Inst Modern Phys, Lanzhou 730000, Gansu, Peoples R China

[2] GSI Helmholtzzentrum Schwerionenforsch GmbH, Planck Str 1, D-64291 Darmstadt, Germany

来源：

VACUUM | 2019年 / 163卷

基金：

中国国家自然科学基金;

关键词：

HIAF; Charge exchange; Dynamic vacuum; StrahlSim;

D O I：

10.1016/j.vacuum.2019.02.004

中图分类号：

T [工业技术];

学科分类号：

08 ;

摘要：

The High-Intensity Heavy Ion Accelerator Facility (HIAF) will provide intermediate charge state ion U-238(35+) with intensity up to 2 x 10(11) particle per pulse (ppp) to different experiments. However, large dynamic vacuum pressure rises of orders of magnitude, caused by lost heavy ions can seriously limit the maximum ion intensity and beam lifetime. Therefore, in order to predict the dynamic vacuum effects induced by the ionization beam loss for the BRing in the HIAF project, a new simulation program (ColBeam) has been developed together with GSI's simulation code StrahlSim are both conducted. The calculation algorithm for dynamic vacuum effect is introduced in this paper. According to the simulation result, up to 3 x 10(11) ppp U-238(35+) particles can be extracted for the current designed BRing vacuum and collimation system, which testifies the rationality of the system design and achieves the requirements of the physics experiments. Higher beam intensity can reach to 5 x 10(11) ppp if the Non-Evaporable Getter (NEG) coating technology is implemented on the dipole and quad-rupole chamber to further suppress the dynamic vacuum effect. The total vacuum pressure evolution with time in the BRing is shown in three-dimensional figure to explain the dynamic vacuum effect induced by the charge exchanged beam loss. The self-developed simulation program was implemented at 320 kV high voltage platform in IMP to simulate the dynamic vacuum evolution and compared with the measured vacuum pressure. Based on the simulation and benchmark results with the experimental data, it is concluded that the software can be used to confirm that dynamic vacuum effect can be suppressed by the collimation system and high speed pump distribution in the BRing.

引用

页码：15 / 25

页数：11

共 50 条

[31] Numerical simulation of high-intensity metal ion beam generation
Koval, T. V.
Ryabchikov, A. I.
Tran My Kim An
Shevelev, A. R.
Sivin, D. O.
Ivanova, A. I.
Paltsev, D. M.
6TH INTERNATIONAL CONGRESS ENERGY FLUXES AND RADIATION EFFECTS, 2018, 1115
[32] The Heavy Ion Accelerator Facility: Research Achievements and Aspirations
Stuchbery, Andrew E.
HEAVY ION ACCELERATOR SYMPOSIUM (HIAS 2019), 2020, 232
[33] High intensity proton accelerator facility in Japan
Mori, Y
HIGH INTENSITY AND HIGH BRIGHTNESS HADRON BEAMS, 2002, 642 : 23 - 28
[34] A Pirani gauge in a high-intensity proton accelerator
Ogiwara, N. (ogiwara.norio@jaea.go.jp), 2012, Elsevier Ltd (86)
[35] Sputtering of targets in high-intensity heavy-ion beam experiments
Sagaidak, R. N.
RADIATION EFFECTS AND DEFECTS IN SOLIDS, 2024,
[36] A Pirani gauge in a high-intensity proton accelerator
Ogiwara, Norio
Hikichi, Yusuke
Kuroiwa, Masahide
VACUUM, 2012, 86 (07) : 908 - 912
[37] THE PROPERTIES OF HIGH-INTENSITY HEAVY-NEGATIVE-ION SOURCE, NIABNIS
TSUJI, H
ISHIKAWA, J
MAEKAWA, T
TAKAGI, T
REVIEW OF SCIENTIFIC INSTRUMENTS, 1990, 61 (01): : 427 - 429
[38] Beam loss studies in high-intensity heavy-ion linacs
Ostroumov, PN
Aseev, VN
Mustapha, B
PHYSICAL REVIEW SPECIAL TOPICS-ACCELERATORS AND BEAMS, 2004, 7 (09): : 1 - 18
[39] HIGH-INTENSITY ELECTRON ACCELERATOR RADIATION HAZARDS
ENGELKE, MJ
PARKER, JR
HEALTH PHYSICS, 1971, 21 (06): : 52 - +
[40] Materials and processing of vacuum components for the high-intensity proton beam accelerator, J-PARC
Saito, Y
VACUUM, 2004, 73 (02) : 181 - 186

← 1 2 3 4 5 →