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Touschek lifetime study based on the precise bunch-by-bunch BCM system at SSRF 被引量:2
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作者 Fang-Zhou Chen Zhi-Chu Chen +4 位作者 Yi-Mei Zhou Ning Zhang Bo Gao Xing-Yi Xu Yong-Bin Leng 《Nuclear Science and Techniques》 SCIE CAS CSCD 2019年第9期126-133,共8页
Continuous tracking of bunch charges is the key to maintain stable operations in a storage ring in top-up mode. Recently, a precise bunch-by-bunch beam-current measurement (BCM) system has been developed at the Shangh... Continuous tracking of bunch charges is the key to maintain stable operations in a storage ring in top-up mode. Recently, a precise bunch-by-bunch beam-current measurement (BCM) system has been developed at the Shanghai Synchrotron Radiation Facility. To avoid the influence of longitudinal oscillation on the amplitudes of the sampling points, a method called two-point equilibrium sampling is introduced. The results, obtained during routine operation time, show that the relative resolution of the measurement of the bunch charges is better than 0.02%. With this high resolution, the new BCM system is able to monitor the bunch-by-bunch beam lifetime. By using the filling pattern information, the Touschek lifetime and the vacuum lifetime can also be calculated. In this paper, the principle of the new method and the experiments is presented in detail. 展开更多
关键词 Beam-current measurement Bunch-bybunch touschek LIFETIME Vacuum LIFETIME SSRF
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BEPCⅡ束流相关本底的蒙特卡罗模拟研究(Ⅲ)——Touschek效应 被引量:3
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作者 金大鹏 过雅南 +4 位作者 王贻芳 伍灵慧 刘振安 赵棣新 郁忠强 《高能物理与核物理》 CSCD 北大核心 2006年第5期449-453,共5页
介绍了Touschek效应本底研究的意义、Touschek效应的作用原理和建模方法.使用自主开发及通用的模拟工具,系统研究了BEPCⅡ工作条件下BESⅢ主要探测器的Touschek本底.模拟和计算束流寿命的比较表明当前的模拟结果是有参考价值的,建模... 介绍了Touschek效应本底研究的意义、Touschek效应的作用原理和建模方法.使用自主开发及通用的模拟工具,系统研究了BEPCⅡ工作条件下BESⅢ主要探测器的Touschek本底.模拟和计算束流寿命的比较表明当前的模拟结果是有参考价值的,建模方法是可行的.探测器的模拟结果表明 Touschek本底不会影响将来BESⅢ的正常稳定运行,不会造成探测器的辐照损伤. 展开更多
关键词 touschek效应 单丝计数率 辐射剂量 本底
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合肥先进光源光束线站辐射源项分析与屏蔽设计验证
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作者 陈家铎 蒋诗平 +2 位作者 赵扬 杨鹏辉 王琳 《强激光与粒子束》 北大核心 2025年第10期225-233,共9页
合肥先进光源作为国际领先的第四代同步辐射光源之一,在束流亮度和相干性方面实现了显著提升,同时也对辐射防护提出了更高要求。传统的辐射屏蔽设计方法主要基于前三代光源的辐射特性,难以满足新一代光源的辐射防护需求,尤其对Touschek... 合肥先进光源作为国际领先的第四代同步辐射光源之一,在束流亮度和相干性方面实现了显著提升,同时也对辐射防护提出了更高要求。传统的辐射屏蔽设计方法主要基于前三代光源的辐射特性,难以满足新一代光源的辐射防护需求,尤其对Touschek效应诱发的固体轫致辐射评估存在明显不足。针对现有研究的局限性,以合肥先进光源的BL10光束线站作为研究对象,针对其复杂的光路结构和频繁切换的运行模式,构建了一个多物理场耦合的模拟分析框架。该框架通过ELEGANT模拟Touschek效应引起的束流损失,利用FLUKA评估辐射传输和能量沉积过程,并借助STAC8计算同步辐射剂量分布,系统分析了各类辐射源的贡献。研究结果表明,Touschek效应对四代光源光束线站的辐射贡献不可忽视,且不同线站间存在显著差异,应在辐射屏蔽设计中予以充分考虑。提出的方法已应用于合肥先进光源光束线站的辐射屏蔽设计与验证,也为新一代光源的辐射防护研究提供了重要参考。 展开更多
关键词 合肥先进光源 光束线站 FLUKA 托歇克效应 轫致辐射
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Experimental study using Touschek lifetime as machine status flag in SSRF
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作者 陈之初 冷用斌 +2 位作者 袁任贤 阎映炳 俞路阳 《Chinese Physics C》 SCIE CAS CSCD 2014年第7期117-122,共6页
The stabilities of the beam and machine have almost the highest priority in a modern light source. Although a lot of machine parameters could be used to represent the beam quality, there is no single parameter that co... The stabilities of the beam and machine have almost the highest priority in a modern light source. Although a lot of machine parameters could be used to represent the beam quality, there is no single parameter that could indicate the global information for the machine operators and accelerator physicists. For the last few years, a new parameter has been studied as a beam quality flag in the Shanghai Synchrotron Radiation Facility (SSRF). Calculations, simulations and detailed analysis of the real-time data from the storage ring have been made and the interesting results have confirmed its feasibility. 展开更多
关键词 touschek lifetime beam quality storage ring
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Tuning control system of a third harmonic superconducting cavity in the Shanghai Synchrotron Radiation Facility 被引量:5
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作者 Peng-Peng Gong Yu-Bin Zhao +6 位作者 Hong-Tao Hou Zhi-Gang Zhang Xiang Zheng Xiao-Yun Pu Kai Xu Qiang Chang Jian-Fei Liu 《Nuclear Science and Techniques》 SCIE CAS CSCD 2019年第10期123-132,共10页
Beam lifetime is dominated by Touschek scattering at the Shanghai Synchrotron Radiation Facility(SSRF).Touschek loss rate is affected by probability for scattering beyond the RF acceptance and the volume charge densit... Beam lifetime is dominated by Touschek scattering at the Shanghai Synchrotron Radiation Facility(SSRF).Touschek loss rate is affected by probability for scattering beyond the RF acceptance and the volume charge density of the bench.In the phaseⅡupgrade of the SSRF,a third harmonic superconducting cavity will be used to enhance the Touschek lifetime by lengthening the bunches.The Touschek lifetime improvement factor is affected by the voltage of a harmonic cavity.To stabilize the cavity voltage,a tuning control system was designed to control it.The design of the tuning control system was based on the SSRF third-generation low-level RF control system.Some hardware and specialized algorithms were redesigned to fit the harmonic cavity control.The design of the tuning control system is complete,and the control system has been tested.The test result shows that the fluctuation of amplitude is<±0.34%within 1.5 h,which satisfies the stability requirement. 展开更多
关键词 Passive HARMONIC CAVITY Low-level radio frequency SHANGHAI SYNCHROTRON Radiation Facility touschek LIFETIME
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Intra-beam scattering and beam lifetime in a candidate lattice of the soft X-ray diffraction-limited storage ring for the upgraded SSRF 被引量:6
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作者 Xin-Zhong Liu Shun-Qiang Tian +2 位作者 Xu Wu Meng Wang Zhen-Tang Zhao 《Nuclear Science and Techniques》 SCIE EI CAS CSCD 2021年第8期57-66,共10页
New-generation synchrotron light sources are being designed and operated worldwide to provide brighter radiation by reducing the beam emittance to X-ray diffraction limits.Intra-beam scattering(IBS)and Touschek scatte... New-generation synchrotron light sources are being designed and operated worldwide to provide brighter radiation by reducing the beam emittance to X-ray diffraction limits.Intra-beam scattering(IBS)and Touschek scattering in such facilities are significant and require attention because of their ultra-low emittance.Therefore,cure strategies need to be carefully studied to obtain highquality photon beams.For the Shanghai Synchrotron Radiation Facility Upgrade(SSRF-U),a candidate lattice of the storage ring,reaching the soft X-ray diffraction limit,was designed and presented for the first time in this study.The emittance growth and beam lifetime in the SSRF-U storage ring were studied using particle simulations for a series of different machine configurations.The gains with RF frequencies of 100 MHz and 500 MHz were compared.Along with a better filling pattern,a more suitable RF frequency was adopted in the SSRF-U.The variations in the equilibrium beam emittance with beam coupling and bunch-lengthening were identified using simulations.Optimal beam coupling and required bunch-lengthening for the SSRF-U storage ring were thus determined.The fitness of the beam energy in the SSRF-U was subsequently assessed using the obtained parameters.Additionally,the Touschek scattering and beam lifetime were calculated,and an acceptable total beam lifetime was obtained. 展开更多
关键词 Diffraction-Limited Storage Ring(DLSR) Shanghai Synchrotron Radiation Facility Upgrade(SSRFU) Intra-Beam Scattering(IBS) touschek scattering Beam lifetime
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合肥光源高亮度运行模式的动力学孔径研究与束流寿命的计算
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作者 周安奇 李永军 +2 位作者 李为民 金玉明 刘祖平 《中国科学技术大学学报》 CAS CSCD 北大核心 1999年第4期491-496,共6页
合肥光源二期工程中注入系统改造后,凸轨系统的所有元件放置在同一个长直线节,这样增加了两块色品校正六极铁,动力学孔径有明显的增大,若色品校正六极铁从原来的两组改为三组,则动力学孔径会进一步增大.计算也表明,当高频电压从... 合肥光源二期工程中注入系统改造后,凸轨系统的所有元件放置在同一个长直线节,这样增加了两块色品校正六极铁,动力学孔径有明显的增大,若色品校正六极铁从原来的两组改为三组,则动力学孔径会进一步增大.计算也表明,当高频电压从原来的0 .1 M V 提高到0 .2 M V。 展开更多
关键词 亮度 动力学孔径 束流寿命 同步辐射光源
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上海光源谐波腔系统的前端变频模块方案设计 被引量:8
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作者 宫鹏鹏 赵玉彬 +6 位作者 侯洪涛 张志刚 郑湘 徐凯 常强 夏洋洋 刘建飞 《核技术》 CAS CSCD 北大核心 2019年第1期1-6,共6页
上海光源是第三代同步辐射光源。在上海光源的二期工程中,超导三次谐波腔将用于拉伸束团长度,提升束流托歇克寿命。三次谐波腔工作在被动模式下,谐波腔工作频率(约1.5 GHz)为主腔工作频率(约500 MHz)的三倍。为实现谐波腔高频系统的调... 上海光源是第三代同步辐射光源。在上海光源的二期工程中,超导三次谐波腔将用于拉伸束团长度,提升束流托歇克寿命。三次谐波腔工作在被动模式下,谐波腔工作频率(约1.5 GHz)为主腔工作频率(约500 MHz)的三倍。为实现谐波腔高频系统的调谐控制,需要对1.5 GHz信号进行下变频处理,便于后端对信号采样处理。本文介绍了三种下变频的方案,将1.5 GHz射频信号降频为31.25 MHz中频信号,分析了各个方案的特点和影响下变频结果的因素。测试结果显示:三种变频方案在不同的动态范围具有良好的线性,均已满足谐波腔控制需求。其中基于倍频器的变频模块为最优方案,其线性动态区间大于70 dB,同时产生的中频信号的相位噪声最低,最终将在谐波腔的控制系统中采用。 展开更多
关键词 三次谐波腔 下变频 低电平 托歇克寿命
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合肥光源托歇克效应损失电子的探测 被引量:4
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作者 孙玉聪 蓝杰钦 +2 位作者 张剑锋 徐宏亮 孙葆根 《强激光与粒子束》 EI CAS CSCD 北大核心 2011年第3期770-774,共5页
束流寿命是衡量储存环性能的重要参数,直接影响着光源的正常运行。对于合肥光源(HLS),托歇克(Touschek)寿命是影响束流寿命的重要因素。为了研究Touschek寿命,需要探测由于Touschek效应所损失的电子。介绍了束流寿命的概念,说明了Tousc... 束流寿命是衡量储存环性能的重要参数,直接影响着光源的正常运行。对于合肥光源(HLS),托歇克(Touschek)寿命是影响束流寿命的重要因素。为了研究Touschek寿命,需要探测由于Touschek效应所损失的电子。介绍了束流寿命的概念,说明了Touschek效应的原理和机制,利用蒙特卡罗软件EGSnrc模拟计算了丢失电子与真空壁的相互作用,通过塑料闪烁体探测器和光电倍增管获得了由于Touschek效应丢失的电子所产生的信号,然后将信号经过放大甄别和符合处理后,用计数器测量了计数率。结果表明:由于Touschek效应而成对丢失的电子的确存在,且电子损失率随流强的降低而减小。这为下一步储存环的能量标定工作做好了前期准备。 展开更多
关键词 合肥光源 束流寿命 托歇克效应 蒙特卡罗方法 塑料闪烁体探测器
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Conceptual design report of the Super Tau-Charm Facility:the accelerator
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作者 Xiao-Cong Ai Liu-Pan An +451 位作者 Shi-Zhong An Yu Bai Zheng-He Bai Olga Bakina Jian-Cong Bao Varvara Batozskaya Anastasios Belias Maria Enrica Biagini Li-Gong Bian Denis Bodrov Anton Bogomyagkov Manuela Boscolo Igor Boyko Ze-Xin Cao Serkant Cetin Marina Chadeeva Ming-Xuan Chang Qin Chang Dian-Yong Chen Fang-Zhou Chen Hai Chen Hua-Xing Chen Jin-Hui Chen Long Chen Long-Bin Chen Qi Chen Qu-Shan Chen Shao-Min Chen Wei Chen Ying Chen Zhi Chen Shan Cheng Si-Bo Cheng Tong-Guang Cheng Lian-Rong Dai Ling-Yun Dai Xin-Chen Dai Achim Denig Igor Denisenko Denis Derkach Heng-Tong Ding Ming-Hui Ding Xiao Ding Liao-Yuan Dong Yong Du Prokhor Egorov Kuan-Jun Fan Si-Yuan Fan Shuang-Shi Fang Zhu-Jun Fang Song Feng Xu Feng Hai-Bing Fu Jun Gao Yuan-Ning Gao Zi-Han Gao Cong Geng Li-Sheng Geng Hai-Liang Gong Jia-Ding Gong Li Gong Shao-Kun Gong Sergi Gonzàlez-Solís Bo-Xing Gou Duan Gu Hao Guo Jun Guo Teng-Jun Guo Xin-Heng Guo Yu-Hui Guo Yu-Ping Guo Zhi-Hui Guo Selcuk Haciomeroglu Eiad Hamwi Cheng-Dong Han Ting-Ting Han Xi-Qing Hao Chong-Chao He Ji-Bo He Tian-Long He Xiao-Gang He Masahito Hosaka Kai-Wen Hou Zhi-Long Hou Dong-Dong Hu Hai-Ming Hu Hao Hu Qi-Peng Hu Tong-Ning Hu Xiao-Cheng Hu Yu Hu Zhen Hu Da-Zhang Huang Fei Huang Guang-Shun Huang Liang-Sheng Huang Peng-Wei Huang Rui-Xuan Huang Xing-Tao Huang Xue-Lei Huang Zhi-Cheng Huang Wang Ji Peng-Kun Jia Sen Jia Ze-Kun Jia Hong-Ping Jiang Hou-Bing Jiang Jian-Bin Jiao Ming-Jie Jin Su-Ping Jin Yi Jin Daekyoung Kang Xian-Wei Kang Xiao-Lin Kang Leonid Kaptari Onur Bugra Kolcu Ivan Koop Evgeniy Kravchenko Yury Kudenko Meike Küßner Yong-Bin Leng Eugene Levichev Chao Li Chun-Yuan Li Chun-Hua Li Hai Tao Li Hai-Bo Li Hang-Zhou Li Heng-Ne Li Hong-Lei Li Hui-Jing Li Hui-Lin Li Jia-Rong Li Jin Li Lei Li Min Li Pei-Rong Li Pei-Lian Li Ren-Kai Li Sang-Ya Li Shu Li Teng Li Tian-You Li Wei-Wei Li Wen-Jun Li Xin Li Xin-Qiang Li Xin-Bai Li Xuan Li Xun-Feng Li Yan-Feng Li Ya-Xuan Li Ying Li Yu-Bo Li Jian Liang Xiao Liang Yu Liang Ze-Rui Liang Chuang-Xin Lin De-Xu Lin Ting Lin Yu-Gen Lin Chao Liu Chao Liu Chia-Wei Liu Gang-Wen Liu Hang Liu Hong-Bang Liu Jian-Bei Liu Jian-Dang Liu Lang-Tian Liu Liang-Chen Liu Ming-Yi Liu Shu-Bin Liu Tao Liu Tian-Bo Liu Xiang Liu Xiao-Yu Liu Xin Liu Xu-Yang Liu Yan-Rui Liu Yan-Lin Liu Yan-Wen Liu Yi Liu Yuan Liu Zhan-Wei Liu Zhao-Feng Liu Zhi-Qing Liu Zi-Rui Liu Zuo-Wei Liu Cai-Dian Lu Miao-Ran Lu Peng-Cheng Lu Yu Lu Qing Luo Tao Luo Tao Luo Xiao-Feng Luo Hui-Hui Lv Shuo-Tian Lyu Xiao-Rui Lyu Bo-Qiang Ma Cheng-Long Ma Shao-Hang Ma Teng Ma Wen-Bin Ma Yu Meng Meng-Xu Fan Xue-Ce Miao Mauro Migliorati Catia Milardi Taisiya Mineeva Yi-Hao Mo Hector Gisbert Mullor Elaf Musa Satoshi Nakamura Alexey Nefediev Yuan-Cun Nie Kazuhito Ohmi MPadmanath Pavel Pakhlov Jian Pang Emilie Passemar Guo-Xi Pei Hua Pei Hai-Ping Peng Liang Peng Rong-Gang Ping Bernard Pire Vindhyawasini Prasad Bin-Bin Qi Zhi-Jun Qi Yi Qian Cong-Feng Qiao Jia-Jia Qin Long-Yu Qin Qin Qin Xiao-Shuai Qin Fedor Ratnikov Craig Roberts Antonio Rodríguez-Sánchez Yury Rogovsky Platon Rogozhin Pablo Roig Man-Qi Ruan Jorge Segovia Feng-Lei Shang Lei Shang Jian-Feng Shangguan Ding-Yu Shao Ming Shao Zhuo-Xia Shao Cheng-Ping Shen Hong-Fei Shen Xiao-Min Shen Zhong-Tao Shen Cai-Tu Shi Jia-Lei Shi Rui-Xiang Shi Yu-Kun Shi Zong-Guo Si Luiz Vale Silva Mikhail Skamarokha Jun-Chao Su Guang-Bao Sun Jun-Feng Sun Kun Sun Li Sun Ming-Kai Sun Rui Sun Xu-Lei Sun Jing-Yu Tang Yin-Gao Tang Ze-Bo Tang Wei Tao Valery Telnov Jia-Xiu Teng Yuriy Tikhonov Cheng-Ying Tsai Timofey Uglov Vincenzo Vagnoni German Valencia Guan-Yue Wan An-Xin Wang Bin Wang Cheng-Zhe Wang En Wang Hong-Jin Wang Jia Wang Jie Wang Jun-Zhang Wang Lei Wang Lei Wang Lin Wang Qian Wang Qian Wang Sheng-Quan Wang Sheng-Yuan Wang Shi-Kang Wang Wei Wang Wei-Ping Wang Xiang-Peng Wang Xia-Yu Wang Xiong-Fei Wang Ya-Qian Wang Yu-Ming Wang Yu-Hao Wang Zeren Simon Wang Zhi Wang Zhi-Gang Wang Zhi-Yong Wang Zi-Yu Wang Zi-Rui Wang Bing-Feng Wei Shao-Qing Wei Shu-Yi Wei Xiao-Min Wei Ya-Jing Wei Ye-Long Wei Ulrich Wiedner Jia-Jun Wu Jun Wu Qun Wu Sang Wu Xin Wu Xing-Gang Wu Xuan Wu Yong-Cheng Wu Yu-Sheng Wu Lei Xia Zhi-Gang Xiao Chun-Jie Xie Kai-Bo Xie Zi-Yu Xiong Ji Xu Lai-Lin Xu Shu-Sheng Xu Xin Xu Yue Xu Liang Yan Wen-Biao Yan Xue-Qing Yan Chi Yang Hai-Jun Yang Hong-Tao Yang Jun Yang Peng-Hui Yang Shuai Yang Tao Yang Wei-Hua Yang Xing-Hua Yang Xue-Ting Yang Yue-Ling Yang Zhen-Wei Yang Zhong-Juan Yang De-Liang Yao Zao-Chen Ye Kai Yi Li Yi Li-Xin Yin Zheng-Yun You Chen Yu Ze Yu Jing Yuan You-Jin Yuan Nefedov Yury Yi-Feng Zeng Wang-Mei Zha Ai-Lin Zhang Ding-Yue Zhang Guang-Yi Zhang Guo-Heng Zhang Hai-Yan Zhang Hao-Ran Zhang Hong-Hao Zhang Hui-Bin Zhang Jia-Lian Zhang Jian-Rong Zhang Jian-Hui Zhang Jian-Yu Zhang Jie-Lei Zhang Lei Zhang Liang Zhang Ling-Hua Zhang Lin-Hao Zhang Ning Zhang Qiu-Yan Zhang Quan-Zheng Zhang Rui Zhang Rui-Yang Zhang Shao-Ru Zhang Sheng-Hui Zhang Shu-Lei Zhang Wen-Chao Zhang Xiao-Yang Zhang Xiao-Ming Zhang Xiao-Tao Zhang Xin Zhang Xin-Hui Zhang Yan-Xi Zhang Ya-Teng Zhang Yi-Hao Zhang Yi-Fei Zhang Yu Zhang Yu Zhang Yu-Mei Zhang Zhen-Yu Zhang Zhi-Qing Zhang Zhi-Cai Zhang Jia-Yao Zhao Ming-Gang Zhao Qiang Zhao Rui-Guang Zhao Yang-Cheng Zhao Ze-Xuan Zhao Zheng-Guo Zhao Alexey Zhemchugov Bo Zheng Jing-Xin Zheng Liang Zheng Ran Zheng Xu-Chang Zheng Yang-Heng Zheng Bin Zhong Dai-Cui Zhou De-Min Zhou Hang Zhou Hao Zhou Jian Zhou Jian-Xin Zhou Qin-Song Zhou Shi-Yu Zhou Xiang Zhou Xiao-Kang Zhou Xiao-Rong Zhou Ya-Jin Zhou Yi Zhou Yi-Mei Zhou Ze-Ran Zhou Bing Zhu Jing-Yu Zhu Jing-Ya Zhu Lin Zhu Rui-Lin Zhu Xing-Hao Zhu Ying-Chun Zhu Zian Zhu Mikhail Zobov Yang Zong Bing-Song Zou Ye Zou Jian Zu 《Nuclear Science and Techniques》 2025年第12期8-177,共170页
Electron-positron colliders operating in the GeV center-of-mass range,or tau-charm energy region,have been proved to enable competitive frontier research due to several unique features.With the progress of high-energy... Electron-positron colliders operating in the GeV center-of-mass range,or tau-charm energy region,have been proved to enable competitive frontier research due to several unique features.With the progress of high-energy physics in the last two decades,a new-generation Tau-Charm factory,called the Super Tau-Charm Facility(STCF),has been actively promoted by the particle physics community in China.STCF has the potential to address fundamental questions such as the essence of color confinement and the matter-antimatter asymmetry within the next decades.The main design goals of the STCF are a center-of-mass energy ranging from 2 to 7 GeV and a luminosity surpassing 5×10^(34)cm^(−2)s^(−1)that is optimized at a center-of-mass energy of 4 GeV,which is approximately 50 times that of the currently operating Tau-Charm factory-BEPCII.The STCF accelerator has two main parts:a double-ring collider with a crab-waist collision scheme and an injector that provides top-up injections for both electron and positron beams.As a typical third-generation electron-positron circular collider,the STCF accelerator faces many challenges in both accelerator physics and technology.In this paper,the conceptual design of the STCF accelerator complex is presented,including the ongoing efforts and plans for technological research and develop-ment,as well as the required infrastructure.The STCF project aims to secure support from the Chinese central government for its construction during the 15th Five-Year Plan(2026-2030). 展开更多
关键词 Third-generation electron-positron collider Super high-luminosity Tau-charm physics Crab-waist collision scheme touschek lifetime
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上海光源储存环束流托歇克寿命研究(英文) 被引量:10
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作者 姜伯承 赵振堂 刘桂民 《高能物理与核物理》 EI CSCD 北大核心 2006年第7期693-698,共6页
上海同步辐射装置(SSRF)是目前在建的第3代专用同步辐射光源.其储存环电子能量3.5GeV,设计束团发射度3.9nm·rad.托歇克寿命将是影响束流寿命的最主要因素,它主要受限于储存环的能量接受度.储存环的能量接受度不但取决于高频电... 上海同步辐射装置(SSRF)是目前在建的第3代专用同步辐射光源.其储存环电子能量3.5GeV,设计束团发射度3.9nm·rad.托歇克寿命将是影响束流寿命的最主要因素,它主要受限于储存环的能量接受度.储存环的能量接受度不但取决于高频电压,同时也受动力学孔径和物理孔径的影响.因此能量接受度的计算将是复杂的.通过计算机模拟跟踪的方法计算储存环各点的能量接受度,其程序是建立在Accelerator Toolbox(AT)基础上的自编程序.通过这些能量接受度数据给出更加准确的托歇克寿命,并且分析了感兴趣的不同运行条件下的托歇克寿命的变化情况. 展开更多
关键词 上海光源 托歇克寿命 能量接受度 模拟跟踪
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Theoretical analysis of BLM system for HLS Ⅱ
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作者 陈裕凯 李裕熊 +1 位作者 李为民 何丽娟 《Chinese Physics C》 SCIE CAS CSCD 2015年第1期83-86,共4页
Hefei Light Source (HLS) is being upgraded to HLS Ⅱ. Its emittance will be much lower than before, therefore the Touschek scattering will increase significantly and become the dominant factor of beam loss. So it is... Hefei Light Source (HLS) is being upgraded to HLS Ⅱ. Its emittance will be much lower than before, therefore the Touschek scattering will increase significantly and become the dominant factor of beam loss. So it is necessary to build a new beam loss monitoring (BLM) system that, in contrast to the old one, is able to obtain the quantity and position information of lost electrons. This information is useful in the commissioning, troubleshooting, and beam lifetime studying for HLS Ⅱ. This paper analyzes the distribution features of different kinds of lost electrons, introduces the operation parameters of the new machine and discusses how to choose proper monitoring positions. Based on these comprehensive analyses, a new BLM system for HLS Ⅱ is proposed. 展开更多
关键词 storage ring beam loss beam lifetime touschek lifetime
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Bunch length manipulation in a diffraction-limited storage ring
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作者 田赛克 焦毅 王九庆 《Chinese Physics C》 SCIE CAS CSCD 2015年第12期62-66,共5页
In an electron storage ring, the bunch length can be increased or decreased by using harmonic cavities. Taking the High Energy Photon Source as an example, we test the bunch length manipulation with harmonic cavities ... In an electron storage ring, the bunch length can be increased or decreased by using harmonic cavities. Taking the High Energy Photon Source as an example, we test the bunch length manipulation with harmonic cavities in a diffraction-limited storage ring (DLSR). The most important collective effects in a DLSR, intra-beam scattering and Touschek effects, are evaluated for different bunch-length patterns. Our study shows that it is feasible to produce long and short bunches simultaneously in a DLSR, without causing severe emittance growth and reduction in lifetime. 展开更多
关键词 high harmonic cavity diffraction-limited storage ring intra-beam scattering touschek effects
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