Xialing Guan
Tsinghua University
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Featured researches published by Xialing Guan.
7th Int. Particle Accelerator Conf. (IPAC'16), Busan, Korea, May 8-13, 2016 | 2016
Tang Ruo; Lei Du; Taibin Du; Weiqiang Guan; Xialing Guan; Yu He; Jian Li; Chuanxiang Tang; Ruo Tang; Xuewu Wang; Qingzi Xing; Huayi Zhang; Qingzhu Zhang
Xi`an Proton Application Facility (XiPAF) is a new proton project which is being constructed for singleevent-effect experiments. It provides proton beam with the maximum energy of 230MeV. The accelerator facility of XiPAF mainly contains a 7MeV Hlinac injector [1] and a proton synchrotron accelerator. The 7MeV Hlinac injector is composed of an ECR ion source, a Low Energy Beam Transport line (LEBT), a Radio Frequency Quadrupole accelerator (RFQ) and a Drift Tube Linac (DTL). The 50keV 10mA Hbeam (pulse width of 1ms) extracted from the ion source is expected to be symmetric transversely with the Twiss parameters Į=0 and ȕ=0.065 mm/mrad. With an adjustable aperture and an electric chopper in the 1.7m-long LEBT, the beam pulse width of 40ȝs and peak current of 6mA can be obtained. The Hbeam is matched into the downstream RFQ accelerator with Į=1.051 and ȕ=0.0494 mm/mrad. This paper presents the detailed design process of the LEBT and the beam dynamics simulation result with the TRACEWIN code. LEBT STRUCTURE In general, Low Energy Transport line (LEBT) is used to match the Hbeam between the Ion source and RFQ accelerator. For the linac injector of Xi`an Proton Application Facility (XiPAF), the beam which is expected to be symmetric transversely is extracted from an ECR ion source. A two-solenoid structure is capable of matching the beam in usual. The RFQ accelerator is expected to accelerate the beam with the pulse width of 40ȝs and input peak current of 6mA, while the Ion Source is designed to produce the beam with the pulse width of 1 ms and peak current of 10 mA. Thus a square aperture and a chopper are inserted into the 1.7m long LEBT. Figure 1 shows the layout of the LEBT. Those elements are related to the beam dynamics. The beam diagnostics devices like faraday cup, ACCT and emittance scanner are included in the design. With the operation experience of the Compact Pulsed Hadron Source (CPHS) at Tsinghua University, it is difficult to manipulate the beam for the field of the solenoids is overlapped with the field of the steering magnets [2]. The rotating of the beam caused by the solenoids couples with the offset of the beam caused by the steering magnets. Therefore, at XiPAF`s linac injector, those two kinds of magnets are set at different position. The beam is focused and steered separately. It is much easier to match the beam in LEBT. The aperture is set after the steering magnets. The off-axis of the beam is avoided at the position of the aperture.
7th Int. Particle Accelerator Conf. (IPAC'16), Busan, Korea, May 8-13, 2016 | 2016
Guangrui Li; Xialing Guan; Xuewu Wang; Zheng Yang; Hongjuan Yao; Qi Zhang; Shuxin Zheng
We have designed a compact proton synchrotron (7∼230 MeV) for applications like proton therapy and space environment study. These applications require slow extraction from 10∼230 MeV. Traditionally, the low energy beam (10∼60 MeV) is achieved by energy degradation from high energy beam which may cause beam lose and energy spread increase, because the beam quality may suffer from magnetic remanence, power ripple and strong space charge effects in low energy stage. To achieve high quality beam directly from resonance extraction, we study these effects by multiparticle simulation. Methods of improving beam quality are discussed.
57th ICFA Advanced Beam Dynamics Workshop on High-Intensity and High-Brightness Hadron Beams (HB'16), Malmö, Sweden, July 3-8, 2016 | 2016
Guangrui Li; Xialing Guan; Wenhui Huang; Xuewu Wang; Zheng Yang; Hongjuan Yao; Hong-jin Zeng; Shuxin Zheng
A compact magnetic alloy (MA) loaded cavity is under development for XiPAF’s synchrotron. The cavity contains 6 large size MA cores, each is independently coupled with solid state power amplifier. Two types of MA core are proposed for the project. We have developed a single core model cavity to verify the impedance model and to test the properties of MA cores under high power state. The high power test results are presented and discussed.
1st International Particle Accelerator Conference, IPAC 2010 | 2010
Jie Wei; Zhi Zeng; Huayi Zhang; Weiqiang Guan; J. E. Stovall; Wenqian Li; Cheng Cheng; Qixi Feng; Zhe Feng; Hongwei Zhao; Shuxin Zheng; C.-K. Loong; Dong Xu; B. Zhong; Beibei Shao; Renkai Li; H. Gong; Yu He; James Billen; Dongsheng Zhang; Xuewu Wang; Guohua Li; Taibin Du; Jian Li; Qingzi Xing; Tianjiao Liang; Xiaofeng Xie; Xialing Guan; Zhanwen Liu; Juzhou Tao
Physics Procedia | 2012
Chun-K. Loong; Jie Wei; Xialing Guan; Xuewu Wang
1st International Particle Accelerator Conference, IPAC 2010 | 2010
Qingzi Xing; Taibin Du; Jian Li; Huayi Zhang; Weiqiang Guan; Yu He; Cheng Cheng; Zhengfeng Xiong; Xialing Guan; J. E. Stovall; L.M. Young; Shuxin Zheng; James Billen; Yujie Bai; Jinchi Cai; Jie Wei
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2012
T.C. Huang; H. Gong; B. Shao; Dong Wang; X.Z. Zhang; K. Zhang; Jie Wei; X.W. Wang; Xialing Guan; C.-K. Loong; Juzhou Tao; L. Zhou; Y.B. Ke
Physics Procedia | 2014
Xuewu Wang; Qingzi Xing; C-K. Loong; Xialing Guan; Taibin Du
Journal of the Korean Physical Society | 2010
Jie Wei; Hb Chen; Cheng Cheng; Qiang Du; Taibin Du; Z. Feng; Xialing Guan; Xiaoxue Han; T.C. Huang; Renkai Li; Wg Li; C.-K. Loong; Bb Sha; Chuanxiang Tang; Qingzi Xing; Yigang Yang; H. Zha; Huayi Zhang; Shuxin Zheng; B. Zhong; Shinian Fu; Juzhou Tao; Yl Zhao; Tianjiao Liang; Liangting Sun; Hw Zhao; Jian Li; Qixi Feng; T Kawai; Gh Li
25th International Linear Accelerator Conference, LINAC 2010 | 2010
Shu Xin Zheng; Xialing Guan; Jie Wei; Huayi Zhang; Jinhai Li; Yaliang Zhao; Jian Li; He Yu; Dongsheng Zhang; James Billen; James Stovall; L.M. Young