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基于角色散诱导微聚束方案的储存环相干光源研究

Toward a storage ring coherent light source based on an angular dispersion-induced microbunching scheme.

作者信息

Li Changliang, Jiang Bocheng, Feng Chao, Gu Qiang, Bai Zhenghe, Wan Weishi, Zhang Qinglei, Wang Kun

机构信息

Shanghai Advanced Research Institute, Chinese Academy of Sciences, Shanghai 201204, People's Republic of China.

Laboratory for Ultrafast Transient Facility, Chongqing University, Chongqing 401331, People's Republic of China.

出版信息

J Synchrotron Radiat. 2025 Jan 1;32(Pt 1):82-89. doi: 10.1107/S1600577524010907.

Abstract

The combination of reversible angular dispersion-induced microbunching (ADM) and the rapid damping storage ring provides a storage-ring-based light source with the capability to produce longitudinal coherent radiation with a high repetition rate. This paper presents a prototype design for a test facility based on the study by Jiang et al. [Sci. Rep. (2022), 12, 3325]. The modulation-demodulation section is inserted into a long straight section of the storage ring instead of a bypass line, which poses great challenges for the optimization of the nonlinear dynamics of the storage ring. However, this design avoids the challenging injection and extraction system connecting to the bypass line. To utilize mature laser technology and reduce the difficulty of the reversible ADM lattice design, we use a long-wavelength 1030 nm seed laser. In the simulation, we achieved 20th harmonic radiation with a bunching factor of about 7.2%. The growth rate of vertical emittance and energy spread of the electron beam for a single pass are about 11% and 0.02%, respectively. When the energy of the electron beam is 800 MeV and two sets of damping wigglers are employed, the damping time in the vertical plane is reduced to 8.31 ms. This results in a 438 kHz repetition rate of the coherent radiation at the new equilibrium state.

摘要

可逆角色散诱导微聚束(ADM)与快速阻尼储存环相结合,提供了一种基于储存环的光源,能够以高重复率产生纵向相干辐射。本文基于Jiang等人的研究[《科学报告》(2022年),12,3325]提出了一种测试设施的原型设计。调制解调部分插入到储存环的长直线段而不是旁路线路中,这给储存环非线性动力学的优化带来了巨大挑战。然而,这种设计避免了连接到旁路线路的具有挑战性的注入和提取系统。为了利用成熟的激光技术并降低可逆ADM晶格设计的难度,我们使用了长波长1030 nm的种子激光。在模拟中,我们实现了20次谐波辐射,聚束因子约为7.2%。电子束单次通过时垂直发射度和能量分散的增长率分别约为11%和0.02%。当电子束能量为800 MeV并采用两组阻尼波荡器时,垂直平面内的阻尼时间缩短至8.31 ms。这导致在新的平衡状态下相干辐射的重复率为438 kHz。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2675/11708862/632d6346e190/s-32-00082-fig1.jpg

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