期刊文献+
共找到10篇文章
< 1 >
每页显示 20 50 100
Conceptual design report of the Super Tau-Charm Facility:the accelerator
1
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
在线阅读 下载PDF
Induced Fission-Like Process of Hadronic Molecular States
2
作者 Jun He dian-yong chen +1 位作者 Zhan-Wei Liu Xiang Liu 《Chinese Physics Letters》 SCIE EI CAS CSCD 2022年第9期6-9,共4页
We predict a new physical phenomenon,induced fission-like process and chain reaction of hadronic molecular states.As a molecular state,if induced by a D meson,the X(3872)can split into D■final state which is forbidde... We predict a new physical phenomenon,induced fission-like process and chain reaction of hadronic molecular states.As a molecular state,if induced by a D meson,the X(3872)can split into D■final state which is forbidden due to the spin-parity conservation.The breeding of the D meson of the reaction,such as D^(0)X(3872)→D^(0)■0D^(0),makes the chain reaction of X(3872)matter possible.We estimate the cross section of the D meson induced fission-like process of X(3872)into two D mesons.With very small D^(0) beam momentum of 1 e V,the total cross section reaches an order of 1000 b,and decreases rapidly with the increasing beam momentum.With the transition of D^(*)meson in molecular states to a D meson,the X(3872)can release large energy,which is acquired by the final mesons.The momentum distributions of the final D mesons are analyzed.In the laboratory frame,the spectator D meson in molecular state concentrates in the low momentum area.The energy from the transition from D^(*)to D meson is mainly acquired by two scattered D mesons.The results suggest that the D meson environment will lead to the induced fission-like process and chain reaction of the X(3827).Such a phenomenon can be extended to other hadronic molecular states. 展开更多
关键词 MESON MOMENTUM BEAM
原文传递
Production of P_(cs)(4459) fromΞ_(b) Decay
3
作者 Qi Wu dian-yong chen Ran Ji 《Chinese Physics Letters》 SCIE CAS CSCD 2021年第7期23-28,共6页
Inspired by the P_(cs)(4459)reported by the LHCb collaboration recently,we investigate the P_(cs)(4459)production from Ξ_(b) decay in a molecular scenario using an effective Lagrangian approach.With different JP assi... Inspired by the P_(cs)(4459)reported by the LHCb collaboration recently,we investigate the P_(cs)(4459)production from Ξ_(b) decay in a molecular scenario using an effective Lagrangian approach.With different JP assignments to P_(cs)(4459),the magnitude of branching fractions of Ξ_(b)→P_(cs)(4459)K is estimated,which is of the order of 10−4.Together with the decay properties of P_(cs)(4459),the present estimations could be further testified by precise measurements and contribute to a better understanding of the molecular interpretations and the exploration of JP quantum numbers of P_(cs)(4459). 展开更多
关键词 DECAY PRECISE branching
原文传递
Light meson emissions of selected charmonium-like states within compact tetraquark configurations
4
作者 李宁 何惠珍 +3 位作者 梁唯 吕齐放 陈殿勇 董宇兵 《Chinese Physics C》 SCIE CAS CSCD 2023年第6期5-14,共10页
We adopt the quark pair creation model to investigate the light meson emissions of several charmoniumlike states.The quark pair creation model is applied to four-body systems,and we calculate the pion/kaon emissions o... We adopt the quark pair creation model to investigate the light meson emissions of several charmoniumlike states.The quark pair creation model is applied to four-body systems,and we calculate the pion/kaon emissions of X(4700),Z_(c)(4430),Y(4230),Y(4360),Y(4390),and Y(4660)within compact tetraquark configurations.We find that the pion/kaon decay widths of X(4700)and Z_(c)(4430)the resonances Y(4230),Y(4360),Y(4390),and Y(4660)cay behaviors will provide useful information for future experimental searches and theoretical interpretations. 展开更多
关键词 charmonium-like states light meson emissions compact tetraquarks strong decays quark pair creation model
原文传递
Production of d_(NΩ)dibaryon in kaon induced reactions
5
作者 刘静 吕齐放 +2 位作者 刘春华 陈殿勇 董宇兵 《Chinese Physics C》 SCIE CAS CSCD 2023年第5期132-138,共7页
In this paper,we propose to investigate the d_(NΩ)dibaryon production in the K-p-→d_(NΩ)≡0 process by utilizing a kaon beam with a typical momentum of approximately 10 GeV,which may be available at COMPASS,OKA@U-7... In this paper,we propose to investigate the d_(NΩ)dibaryon production in the K-p-→d_(NΩ)≡0 process by utilizing a kaon beam with a typical momentum of approximately 10 GeV,which may be available at COMPASS,OKA@U-70,and SPS@CERN.The cross sections for K-p-→d_(NΩ)=O are estimated,and in particular,the magnitude of the cross sections is evaluated to be several hundred nanobarns at Pk=20 GeV.Considering that the d_(NΩ)dibaryon dominantly decays into≡Λand≡∑,we also estimate the cross sections for K-p→≡0Λ≡0 and K~p→≡-∑+≡0,where the d_(NΩ)dibaryon can be observed in the invariant mass distributions of≡0Λand≡-∑+,respectively. 展开更多
关键词 DIBARYON production process Kaon induced reaction
原文传递
Molecular components in J/ψandρ-πpuzzle
6
作者 郭星导 陈殿勇 +2 位作者 李学潜 苑仲元 桑士晶 《Chinese Physics C》 SCIE CAS CSCD 2024年第5期141-150,共10页
Motivated by the large branching fractions of J/ψ→f0(1710)ω/f0(1710)ϕand the light exotic candidates,we found that there may exist molecular states composed of f0(1710)ωand f0(1710)ϕ,which correspond to X(2440)and... Motivated by the large branching fractions of J/ψ→f0(1710)ω/f0(1710)ϕand the light exotic candidates,we found that there may exist molecular states composed of f0(1710)ωand f0(1710)ϕ,which correspond to X(2440)and X(2680)observed a few decades ago.The branching fractions of X(2440)and X(2680)to various PV and KKω(ϕ)channels were estimated in the molecular scenario.In addition,the large branching fractions of J/ψ→f0(1710)ω/f0(1710)ϕindicate sizable molecular components in the J/ψstate.Thus,we consider J/ψas the superposition of thecc¯(1S),f0(1710)ω,and f0(1710)ϕmolecular states.These molecular components have a significant impact on the light hadron decays of J/ψ,which may elucidate the long standingρ−πpuzzle. 展开更多
关键词 ρ-πpuzzle J/Ψ molecular state
原文传递
Radiative decays of charmed mesons in a modified relativistic quark model
7
作者 Jie-Lin Li dian-yong chen 《Chinese Physics C》 SCIE CAS CSCD 2022年第7期56-67,共12页
In this study, we perform systematic estimations of the radiative decays of the charmed mesons in a modified relativistic quark model. Our estimations indicate that the branching ratios of the processes of D^(0)_(2)(1... In this study, we perform systematic estimations of the radiative decays of the charmed mesons in a modified relativistic quark model. Our estimations indicate that the branching ratios of the processes of D^(0)_(2)(1^(3)P_(2)) →D^(0)(1^(3)S_(1)) γ , D_3^0(1D_3) o D^(0)_(2)(1^(3)P_(2)) γ , D^(0)_(2)(2D_2^) o D_1^(0)(2P_1) γ , D_3^0(2^3D_3) o D^(0)_(2)(2^3P_(2)) γ , and D^(\ast 0)(1^(3)S_(1)) o D^0(1^1S_0) γ are of the order of 10^(-2) , which are sizable to be detected experimentally. Moreover, the branching ratios of some channels, for example, D_1^0(1P_1) o D(1^1S_0)^0 γ , D^0(3^1S_0) o D_1^( 0)(2P^_(1)) γ , and D^0(3^3S_(1)) o D^(0)_(2)(2^3P_(2)) γ , are estimated to be of the order of 10^(-3) , which may be accessible with the accumulation of data in future experiments. 展开更多
关键词 charmed mesons radiative decays quark model
原文传递
Molecular picture for X_(0)(2900) and X_(1)(2900)
8
作者 Jun He dian-yong chen 《Chinese Physics C》 SCIE CAS CSCD 2021年第6期23-28,共6页
Inspired by the newly observed X0(2900)and Xj(2900)states at LHCb,the K^(*)D^(*)and KD_(1)interactions are studied in the quasipotential Bethe-Salpeter equation approach combined with the one-boson-exchange model.The ... Inspired by the newly observed X0(2900)and Xj(2900)states at LHCb,the K^(*)D^(*)and KD_(1)interactions are studied in the quasipotential Bethe-Salpeter equation approach combined with the one-boson-exchange model.The bound and virtual states from the interactions are searched for as poles in the complex energy plane of scattering amplitude.A bound state with I(JP)=0(0^(+))and a virtual state with 0(1^(-))are produced from the K^(*)D^(*)interaction and KD_(1)interaction,and can be related to the X_(0)(2900)and Xi(2900)observed at LHCb,respectively.A bound state with I(JP)=0(1^(+))and a virtual state with I(J_(P))=0(2_(+))are also predicted from the KD_(1)interaction,with the same a value,to reproduce the X_(0.1)(2900),which can be searched for in future experiments. 展开更多
关键词 molecular state quasipotential Bethe-Salpeter equation potential model
原文传递
X(2239) and η(2225) as hidden-strange molecular states from Λ Λ interaction
9
作者 Jun-Tao Zhu Yi Liu +2 位作者 dian-yong chen Longyu Jiang Jun He 《Chinese Physics C》 SCIE CAS CSCD 2020年第12期29-37,共9页
In this work,we propose the possible assignment of the newly observed X(2239),as well asη(2225),as a molecular state from the interaction of a baryonΛand an antibaryonΛ.With the help of effective Lagrangians,theΛ... In this work,we propose the possible assignment of the newly observed X(2239),as well asη(2225),as a molecular state from the interaction of a baryonΛand an antibaryonΛ.With the help of effective Lagrangians,theΛΛinteraction is described within the one-boson-exchange model withη,η′,ω,ϕ,andσexchanges considered.After inserting the potential kernel into the quasipotential Bethe-Salpeter equation,the bound states from theΛΛinteraction can be studied by searching for the pole of the scattering amplitude.Two loosely bound states with spin parities I^(G)(J^(PC))=0^(+)(0^(−+))and 0^(−)(1^(−−))appear near the threshold with almost the same parameter.The 0^(−)(1^(−−))state can be assigned to X(2239)observed at BESⅢ,which is very close to theΛΛthreshold.The scalar mesonη(2225)can be interpreted as a 0^(+)(0^(−+))state from theΛΛinteraction.The annihilation effect is also discussed through a coupled-channel calculation plus a phenomenological optical potential.It provides large widths to two bound states produced from theΛΛinteraction.The mass of the 1^(−)state is slightly larger than the mass of the 0^(−)state after including the annihilation effect,which is consistent with our assignment of these two states as X(2239)andη(2225),respectively.The results suggest that further investigation is required to understand the structures near theΛΛthreshold,such as X(2239),η(2225),and X(2175). 展开更多
关键词 hadronic molcular state X(2239) X(2225)
原文传递
Using X(3823)→J/ψπ+π- to identify coupled-channel effects
10
作者 Bo Wang Hao Xu +3 位作者 Xiartg Liu dian-yong chen Susana Coito Estia Eichten 《Frontiers of physics》 SCIE CSCD 2016年第3期151-159,共9页
Very recently, the Belle and BESIII experiments observed a new charmonium-like state X(3823), which is a good candidate for tile D-wave charmonium (13D2). Because the X(3823) is just near the DD* threshold, the... Very recently, the Belle and BESIII experiments observed a new charmonium-like state X(3823), which is a good candidate for tile D-wave charmonium (13D2). Because the X(3823) is just near the DD* threshold, the decay X(3823)→J/ψπ+π- can be a golden channel to test the significance of coupled-channel effects. In this work, this decay is considered including both the hidden-charm dipion and the usual quantum chromodynamics multipole expansion (QCDME) contributions. The partial decay width, the dipion invari^nt mass spectrum distribution dF[X(3823) →J/ψπ+π- /dmπ+π-, and the corresponding dF[X(3823) →J/ψπ+π-/d cosθ distribution are computed. Many param- eters are determined from exi:sting experimental data, so the results depend mainly only on one unknown phase between the QCDME and hidden-charm dipion amplitudes. 展开更多
关键词 CHARMONIUM Hidden-charm dipion decay
原文传递
上一页 1 下一页 到第
使用帮助 返回顶部