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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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ExclusiveΩ^(++)_(ccc)Ω^(--)_(ccc)Production from Z^(0)/r^(*)Decays
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作者 Hong Chen rong-gang ping 《Chinese Physics Letters》 SCIE CAS CSCD 2018年第1期18-21,共4页
Based on the quark model the cross section for the e^(+)e^(-)→Z^(0)/r^(*)→Ω^(++)_(ccc)Ω^(--)_(ccc)exclusive process is investigated at the tree level.Compared with the Z^(0)→Ω^(-)Ω^(+)decay,our result shows tha... Based on the quark model the cross section for the e^(+)e^(-)→Z^(0)/r^(*)→Ω^(++)_(ccc)Ω^(--)_(ccc)exclusive process is investigated at the tree level.Compared with the Z^(0)→Ω^(-)Ω^(+)decay,our result shows that the Z^(0)boson favors decaying into charmed baryon pairs.The results are also compared with the calculation of inclusively charmed baryon production. 展开更多
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Phenomenological study of J/ψ→Ξ^(0)(Λπ^(0))ˉΞ^(0)(Λγ)decays
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作者 洪鹏程 平荣刚 +2 位作者 宋维民 李贺 周小蓉 《Chinese Physics C》 SCIE CAS CSCD 2023年第9期52-60,共9页
The measurement of decay parameters is one of the important goals of particle physics experiments,and the measurement serves as a probe to search for evidence of CP violation in baryonic decays.The experimental result... The measurement of decay parameters is one of the important goals of particle physics experiments,and the measurement serves as a probe to search for evidence of CP violation in baryonic decays.The experimental results will aid in advancing existing theoretical research and establishing new experimental objectives.In this study,we formulate the asymmetric parameters that characterize parity violation,and then derive formulas for the measurement of CP violation.The formulae for the joint angular distribution of the full decay chain as well as the polarization observable of Ξ^(0),Ξ¯^(0),Λ,and Λ¯are also provided for experiments.Lastly,we evaluated the sensitivity of two asymmetric parameters:αΞ0→Λπ0(abbreviated asαΞ0)andαΞ¯0→Λ¯γ(abbreviated asαΞ¯0)for future experimental measurements. 展开更多
关键词 parity violation asymmetry parameters spin density matrix angular distribution sensitivity
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Study of parity violation inΛ^(+)_(c)→ΦρandΛ^(+)_(c)→ωρdecays
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作者 洪鹏程 严芳 +1 位作者 平荣刚 罗涛 《Chinese Physics C》 SCIE CAS CSCD 2023年第5期49-56,共8页
CP violation in baryonic decays has not been significantly observed.With large data events accumulated at e+e-colliders or the Large Hadron Collider,charmed baryon decays would provide a promising laboratory to test C... CP violation in baryonic decays has not been significantly observed.With large data events accumulated at e+e-colliders or the Large Hadron Collider,charmed baryon decays would provide a promising laboratory to test CP symmetry.In this study,we formulateΛ^(+)_(c)→ΦρandΛ^(+)_(c)→ωρdecays for the measurement of their asymmetry parameters in weak decays at the BESII or LHCb experiments.The polarization transfer is analyzed in the two processes of e+e-→Λ^(+)_(c)Λ^(-)_(c)andΛ^(o)_(b)→Λ^(+)_(c)π^(-),and the formulas for the joint angular distribution of these processes are provided.The sensitivity of the measurement of the asymmetry parameters of the above two decay processes is estimated for future experiments. 展开更多
关键词 parity violation asymmetry parameters sensitivity spin density matrix angular distribution
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Polarization in ■ decays
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作者 Tong-Zhu Han rong-gang ping +1 位作者 Tao Luo Guang-Zhi Xu 《Chinese Physics C》 SCIE CAS CSCD 2020年第1期11-15,共5页
Measurements of decay asymmetry parameters of charmed baryons,e.g.,■,provide more data to test the W-emission and W-exchange mechanisms controlled by strong and weak interactions.Taking advantage of the spin polariza... Measurements of decay asymmetry parameters of charmed baryons,e.g.,■,provide more data to test the W-emission and W-exchange mechanisms controlled by strong and weak interactions.Taking advantage of the spin polarization in charmed baryon decays,we investigate the possibility to measure weak decay asymmetry parameters in thee^+e^-→■ process.We analyze the transverse polarization spontaneously produced in this process and the spin transfer in the subsequent■ decays.The sensitivity to measure the asymmetry parameters is estimated for the decay■→■. 展开更多
关键词 transverse polarization asymmetry parameters SPIN charmed baryon decays
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Using A^(+)_(c)→pK^(-)π^(+) as aspin polarimeter
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作者 Dai-Hui Wei Yong-Xu Yang rong-gang ping 《Chinese Physics C》 SCIE CAS CSCD 2022年第7期85-92,共8页
Polarization transfer measurement plays an important role in the search for new physics processes incharmed baryon decays.The measurement of the A^(+)_(c)→pK^(-)π^(+) decay is suggested asaspinpolarimeter.A general ... Polarization transfer measurement plays an important role in the search for new physics processes incharmed baryon decays.The measurement of the A^(+)_(c)→pK^(-)π^(+) decay is suggested asaspinpolarimeter.A general description of the decay is developed using Euler angles,and the polarization parameters are derived.Its relationship with parity violation is found using the phenomenological amplitude model.A Monte-Carlo simulation is performed,and the results show that charmed baryon polarization iswell determined usingaset ofMonte-Carloevents with selected asymmetry parameters.The experimental measurement of these asymmetry parameters is suggested. 展开更多
关键词 A_(c)baryon POLARIZATION
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