Liang Lu
Chinese Academy of Sciences
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Chinese Physics C | 2016
Liang Lu; T. Hattori; H. Y. Zhao; Katsunori Kawasaki; Liepeng Sun; Qianyu Jin; Junjie Zhang; Liangting Sun; Yuan He; Hongwei Zhao
A hybrid single cavity(HSC) linac, which is formed by combining a radio frequency quadrupole(RFQ)and a drift tube(DT) structure into one interdigital-H(IH) cavity, is fabricated and assembled as a proof of principle injector for cancer therapy synchrotron, based on the culmination of several years of research. The HSC linac adopts a direct plasma injection scheme(DPIS), which can inject a high intensity heavy ion beam produced by a laser ion source(LIS). The input beam current of the HSC is designed to be 20 m A C6+ ions. According to numerical simulations, the HSC linac can accelerate a 6-m AC6+ beam, which meets the requirement of the needed particle number for cancer therapy(108-9ions/pulse). The HSC injector with the DPIS method makes the existing multiturn injection system and stripping system unnecessary, and can also bring down the size of the beam pipe in existing synchrotron magnets, which could reduce the whole cost of synchrotron. The radio frequency(rf) measurements show excellent rf properties for the resonator, with a measured Q equal to 91% of the simulated value. AC6+ ion beam extracted from the LIS was used for the HSC commissioning. In beam testing, we found the measured beam parameters agreed with simulations. More details of the measurements and the results of the high power test are reported in this paper.A hybrid single cavity (HSC) linac, which is formed by combining a radio frequency quadrupole (RFQ) and a drift tube (DT) structure into one interdigital-H (IH) cavity, is fabricated and assembled as a proof of principle injector for cancer therapy synchrotron, based on the culmination of several years of research. The HSC linac adopts a direct plasma injection scheme (DPIS), which can inject a high intensity heavy ion beam produced by a laser ion source (LIS). The input beam current of the HSC is designed to be 20 mA C6+ ions. According to numerical simulations, the HSC linac can accelerate a 6-mA C6+beam, which meets the requirement of the needed particle number for cancer therapy (108–9 ions/pulse). The HSC injector with the DPIS method makes the existing multi-turn injection system and stripping system unnecessary, and can also bring down the size of the beam pipe in existing synchrotron magnets, which could reduce the whole cost of synchrotron. The radio frequency (rf) measurements show excellent rf properties for the resonator, with a measured Q equal to 91% of the simulated value. A C6+ ion beam extracted from the LIS was used for the HSC commissioning. In beam testing, we found the measured beam parameters agreed with simulations. More details of the measurements and the results of the high power test are reported in this paper.
Archive | 2015
Zhouli Zhang; Yuan He; Aimin Shi; Liepeng Sun; Xianbo Xu; Longbo Shi; Chenxing Li; Wenbin Wang; Liang Lu; Bin Zhang; Xiaofeng Jin; Jing Wang; Xianwu Wang; Y. Q. Guo; Huan Jia; J. Wu; Hong-Wei Zhao; Yong Liu; D. Li; Chuan Zhang
The injector II RFQ accelerator of ADS is used to accelerate protons of 10 mA from 35 keV to 2.1 MeV. The cavity structure of the RFQ is the same as that of the SNS RFQ which has a square cross section, and it adopts π-mode rods to enhance the RF (radio frequency) stability of the cavity. Low power tests show that the flatness of the cavity is better than ±0.01 and the unloaded Q value is 13000. CW (continuous wave) working condition was realized after a long time conditioning of the cavity. Beam tests were conducted with a current of 10 mA in pulse mode and CW mode, respectively, and it indicates that the transmission efficiency is 95.3%, output energy is 2.165 MeV, energy spread is 1.9%, and the transverse and longitudinal emittances are all 0.33 πmm·mrad. ©, 2015, Atomic Energy Press. All right reserved.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2017
Wei Ma; Liang Lu; Xianbo Xu; Liepeng Sun; Zhouli Zhang; Weiping Dou; Chenxing Li; Longbo Shi; Yuan He; Hongwei Zhao
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2017
Wei Ma; Liang Lu; Ting Liu; Xianbo Xu; Liepeng Sun; Chenxing Li; Longbo Shi; Wenbin Wang; Yuan He; Hongwei Zhao
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2014
Zhouli Zhang; Liepeng Sun; Huan Jia; Yuan He; Aimin Shi; X. F. Du; Jing Wang; Xiaofeng Jin; Gang Pan; Xianbo Xu; Chenxing Li; Longbo Shi; Liang Lu; Z.J. Zhang; J. Wu; Haoning Wang; Tieming Zhu; Xianwu Wang; Y. Q. Guo; Yong Liu; Hongwei Zhao
5th Int. Particle Accelerator Conf. (IPAC'14), Dresden, Germany, June 15-20, 2014 | 2014
Zhouli Zhang; Y. Q. Guo; Yuan He; M. Hoff; Huan Jia; Andrew Lambert; Chenxing Li; D. Li; Yong Liu; Liang Lu; Gang Pan; Aimin Shi; Longbo Shi; John Staples; Liepeng Sun; Steve Virostek; Wenbin Wang; Xianwu Wang; J. Wu; Q. Wu; Xianbo Xu; Bin Zhang; Chuan Zhang; Junhui Zhang; Hong-Wei Zhao; Tieming Zhu
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2018
Wei Ma; Liang Lu; Ting Liu; Longbo Shi; Liepeng Sun; Chenxing Li; Wenbin Wang; Xianbo Xu; Tao He; Yuan He; Hongwei Zhao
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2018
Chenxing Li; Yuan He; Feng-Feng Wang; Peiyan Yu; L. Yang; C. G. Li; Wenbin Wang; Xianbo Xu; Longbo Shi; Wei Ma; Liepeng Sun; Liang Lu; Zhijun Wang; Aimin Shi; Tieshan Wang
Archive | 2017
Wei Ma; Hongwei Zhao; Xianbo Xu; Liepeng Sun; Yuan He; Liang Lu; Zhouli Zhang; Chenxing Li; Longbo Shi
Matter and Radiation at Extremes | 2017
Liang Lu; Wei Ma; Chenxing Li; Tao He; L. Yang; Liepeng Sun; Xianbo Xu; Wenbing Wang; Longbo Shi