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Conceptual design report of the Super Tau-Charm Facility: the accelerator
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Abstract
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 development, 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).
Springer Science and Business Media LLC
Xiao-Cong Ai
Liu-Pan An
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
M. Padmanath
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
Title: Conceptual design report of the Super Tau-Charm Facility: the accelerator
Description:
Abstract
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 development, 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).
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