Design and simulation of beam injection scheme for diffraction limited storage ring
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摘要: 衍射极限储存环（DLSR）作为第四代同步辐射光源，正得到世界各国的大力发展和建设。如何在尽量减小对存储束流扰动情况下，高效率地将束流注入到储存环中，是衍射极限储存环设计与运行中的重要课题之一。传统的局部凸轨注入法有着很长的历史，应用广泛且技术成熟，但是传统凸轨注入法会对存储束流造成扰动，且衍射极限储存环的动力学孔径较小，这给传统凸轨注入法的应用带来了困难。为了解决这些问题，改进了一些传统的离轴注入法，提出并发展了一些在轴的注入方法。合肥先进光源（HALF）是规划建设中的衍射极限储存环光源，基于HALF储存环的物理设计方案，设计并应用了几种离轴或在轴的注入方案，通过粒子跟踪和模拟的方法验证了它们的可行性并研究了注入效率等物理问题，并对模拟结果进行了讨论和总结。Abstract: As the fourth synchrotron radiation light source, diffraction-limited storage rings (DLSRs) are being vigorously developed and constructed around the world. How to efficiently inject beam into the storage ring while minimizing the disturbance to the stored beam is one of the important issues in the design and operation of DLSRs. The conventional bump injection which has a long history is widely used and has mature technology. However, it disturbs the stored beam and the small dynamic aperture of DLSRs, which makes it difficult to apply the conventional bump injection on DLSRs. To solve these problems, some conventional off-axis injection method have been improved and several on-axis injection methods have been proposed and developed. Hefei Advanced Light Facility (HALF) is a DLSR under planning and construction. Based on the physical design of the HALF storage ring, a couple of off-axis or on-axis injection schemes have been designed and applied. Their feasibility has been verified through particle tracking and simulation, and physical issues such as injection efficiency have been studied. Discussion of results and conclusion are also presented.
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图 1 HALF储存环一个周期的lattice及线性光学参数
Figure 1. Magnet layout and linear optical parameters of one period HALF lattice
图 3 采用反向切割磁铁的凸轨注入法的元件布局示意图
Figure 3. Schematic layout of injection devices for the bump injection scheme with anti-septum (K2)
图 8 脉冲多极铁注入法的元件布局示意图
Figure 8. Schematic layout of injection devices for the multipole kicker injection scheme
图 10 注入方案及注入束流首圈运动轨迹
Figure 10. First turn trajectory of the injection particle and specific parameters of the injection scheme
图 12 有误差存在下的脉冲多极铁注入效率
Figure 12. Injection efficiency of pulsed multipole injection with error
图 13 脉冲多极铁注入对存储束流的影响
Figure 13. Influence of pulsed multipole injection on the stored beam
图 14 纵向注入法的元件布局示意图
Figure 14. Schematic layout of injection devices for the longitudinal injection scheme
图 15 纵向注入中纵向相空间上下边界
Figure 15. Upper and lower boundaries of longitudinal phase space in longitudinal injection
图 17 纵向注入束流累积过程
Figure 17. Accumulation process of injection beam in longitudinal injection
表 1 HALF储存环主要设计参数
Table 1. Main parameters of the HALF storage ring
circumference/
mbeam
energy/
GeVfocusing
typenatural
emittance/
(pm·rad)transverse
tunes
(H/V)natural
chromaticities
(H/V)momentum
compaction
factorenergy
loss per
turn/keVharmonic
numberRF
frequency/
MHzRF
voltage/
kVdamping
time
(H/V/L)/msnatural
energy
spread479.86 2.2 20×6BA 86.3 48.15/17.15 −77/−57 9.0×10−5 186.7 800 500 1000 27.2/37.7/23.4 0.62×10−3 
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表 2 脉冲多极铁注入方案主要参数
Table 2. Main parameters of pulsed multipole injection scheme
horizontal position
of the injection beam
at septum/mmincidence angle of
the injection beam
at septum/mradposition
of
septumposition of
nonlinear
kickerlength of
nonlinear
kicker/cmkick angle of
nonlinear
kicker/mrad12 −3.1 midpoint of long
straight sectiondownstream of long
straight section40 3
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表 3 纵向注入方案主要参数
Table 3. Main parameters of longitudinal injection scheme
injection beam time offset/ns injection beam energy offset/% RF frequency/MHz RF voltage/kV harmonic number bunch spacing/ns −5 4.34 100 350 160 10
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[1] Shang L, Shang F L, Lu Y M, et al. The new injection system of the HLS II[C]//Proceedings of the IPAC 2013. 2013: 687-689. [2] Ohkuma H. Top-up operation in light sources[C]//Proceedings of the EPAC08. 2008: 36. [3] Bei M, Borland M, Cai Yongda, et al. The potential of an ultimate storage ring for future light sources[J]. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2010, 622(3): 518-535. [4] Hettel R. DLSR design and plans: an international overview[J]. Journal of Synchrotron Radiation, 2014, 21(Pt 5): 843-855. [5] 焦毅, 白正贺. 第四代同步辐射光源物理设计与优化[J]. 强激光与粒子束, 2022, 34:104004 doi: 10.11884/HPLPB202234.220136Jiao Yi, Bai Zhenghe. Physics design and optimization of the fourth-generation synchrotron light sources[J]. High Power Laser and Particle Beams, 2022, 34: 104004 doi: 10.11884/HPLPB202234.220136 [6] Gough C, Aiba M. Top-up injection with “anti-septum”[C]//Proceedings of the IPAC2017. 2017: 774-776. [7] Harada K, Kobayashi Y, Miyajima T, et al. New injection scheme using a pulsed quadrupole magnet in electron storage rings[J]. Physical Review Special Topics-Accelerators and Beams, 2007, 10: 123501. doi: 10.1103/PhysRevSTAB.10.123501 [8] Takaki H, Nakamura N, Kobayashi Y, et al. Beam injection with a pulsed sextupole magnet in an electron storage ring[J]. Physical Review Special Topics−Accelerators and Beams, 2010, 13: 020705. [9] Takai R, Obina T, Ueda A, et al. Beam profile measurement during top-up injection with a pulsed sextupole magnet[C]//Proceedings of the DIPAC2011. 2011: 305-307. [10] Henderson S. Status of the APS upgrade project[C]//Proceedings of the 6th International Particle Accelerator Conference. 2015: 1791-1793. [11] Steier C, Anders A, Byrd J, et al. ALS-U: a Soft X-ray diffraction limited light source[C]//Proceedings of the 2nd North American Particle Accelerator Conference. 2016. [12] Chen Jinhui, Shi Hengxu, Wang L, et al. Strip-line kicker and fast pulser R&D for the HEPS on-axis injection system[J]. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2019, 920: 1-6. [13] Aiba M, Böge M, Marcellini F, et al. Longitudinal injection scheme using short pulse kicker for small aperture electron storage rings[J]. Physical Review Special Topics−Accelerators and Beams, 2015, 18: 020701. [14] Hernandez A S, Aiba M. Investigation of the injection scheme for SLS 2.0[C]//Proceedings of the 6th International Particle Accelerator Conference. 2015: 1720-1723. [15] Terebilo A. Accelerator toolbox for MATLAB[R]. SLAC-PUB-8732, 2001. [16] 白正贺, 刘刚文, 何天龙, 等. 合肥先进光源储存环初步物理设计[J]. 强激光与粒子束, 2022, 34:104003 doi: 10.11884/HPLPB202234.220137Bai Zhenghe, Liu Gangwen, He Tianlong, et al. Preliminary physics design of the Hefei Advanced Light Facility storage ring[J]. High Power Laser and Particle Beams, 2022, 34: 104003 doi: 10.11884/HPLPB202234.220137 [17] MAX IV detailed design report[EB/OL]. https://www.maxiv.lu.se/accelerators-beamlines/accelerators/accelerator-documentation/max-iv-ddr/. [18] Leemann S C. Pulsed sextupole injection for Sweden’s new light source MAX IV[J]. Physical Review Special Topics-Accelerators and Beams, 2012, 15: 050705. doi: 10.1103/PhysRevSTAB.15.050705 [19] Atkinson T, Dirsat M, Dressler O, et al. Development of a non-linear kicker system to facilitate a new injection scheme for the BESSY II storage ring[C]//Proceedings of the IPAC2011. 2011: 3394-3396. [20] Song Wenbin, Shang Lei, Shang Fenglei, et al. A novel kind of nonlinear kicker for the Hefei Advanced Light Facility[J]. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2021, 990: 164986. [21] Wang P N, Liu G, Wang L, et al. Acceptance analysis method for the scheme design of multipole kicker injection[C]//Proceedings of the 12th International Particle Accelerator Conference. 2021: 2900-2902. [22] Wang L, Chen J H, Shi H, et al. A novel 5-cell strip-line kicker prototype for the HEPS on-axis injection system[J]. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2021, 992: 165040. -
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