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Influence of pre-stretching and annealing on microstructure and mechanical properties evolution of twin-roll cast Mg-2Al-1Zn-1Ca(wt.%)plates 被引量:1
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作者 H.Yu S.J.Niu +8 位作者 c.liu L.P.Tian L.W.Quan Z.K.Liu Y.L.Xu L.X.Huang K.S.Shin W.Yu B.A.Jiang 《Journal of Materials Science & Technology》 2025年第6期171-184,共14页
Pre-stretching and annealing treatments were conducted on twin roll cast Mg-2Al-1Zn-1Ca(AZX211,in wt.%)plates with a rare earth-like texture.Varying amounts of deformation were applied along the rolling direction(RD)a... Pre-stretching and annealing treatments were conducted on twin roll cast Mg-2Al-1Zn-1Ca(AZX211,in wt.%)plates with a rare earth-like texture.Varying amounts of deformation were applied along the rolling direction(RD)and transverse direction(TD)of AZX211 alloy in order to modify its mechanical proper-ties at room temperature.The results demonstrate that pre-stretching treatment effectively enhances the yield strength(YS),especially along the RD.The strengthening mechanism is attributed to the production of a large number of dislocations and sub-grain boundaries,but the work-hardening ability of the plate will be greatly weakened.Additionally,annealing treatment substantially improves the plasticity and in-plane anisotropy and restores the work-hardening ability.The notable distinction in the pre-stretching process between different directions lies in the underlying deformation mechanism.In case of RD,de-formation is predominantly governed by the slip mechanism of{0002}{11−20}basal slip and{10−10}{11−20}prismatic slip,while along the TD,deformation is primarily controlled by{0002}{11−20}basal slip without significant twinning deformation.When a 6%pre-stretching is conducted,the initial rare earth-like texture of the sample transforms into a symmetrically distributed double-peak basal texture,accompanied by grain refinement.This texture transformation is chiefly due to the dominance of{0002}{11−20}basal slip-driven deformation.Moreover,the annealed sample maintains a strong basal texture,owing to strain-induced recrystallization. 展开更多
关键词 Mg alloys PRE-STRETCHING ANNEALING Texture Yield strength
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Low-Cycle Fatigue Properties of Nickel-Based Superalloys Processed by High-Gradient Directional Solidification 被引量:4
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作者 Z.D.Fan D.Wang +4 位作者 c.liu G.Zhang J.Shen L.H.Lou J.Zhang 《Acta Metallurgica Sinica(English Letters)》 SCIE EI CAS CSCD 2017年第9期878-886,共9页
The low-cycle fatigue (LCF) properties of DD10 (single-crystal) and DZ53 (columnar-grained) superalloys solidified by liquid-metal cooling (LMC) and high-rate solidification (HRS) processes have been systema... The low-cycle fatigue (LCF) properties of DD10 (single-crystal) and DZ53 (columnar-grained) superalloys solidified by liquid-metal cooling (LMC) and high-rate solidification (HRS) processes have been systematically investi- gated. It was found that the LCF life of DZ53 solidified by LMC was obviously better than that solidified by HRS. In contrast, for DD10, LMC showed no remarkable influences on LCF properties at high temperature and only improved LCF properties at intermediate temperature. Microstructure examination showed that the cracks generally initiated at microp- ores in the subsurface at intermediate temperature. However, the cracks occurred on the surface due to oxidation, or persistent slip bands near script-MC at high temperature. Therefore, the benefits of LMC technique can be attributed to both of the reduced casting defects which significantly affect the LCF properties at intermediate temperature and the improved microstructural homogeneity which was strongly correlated to the LCF properties of alloys at high temperature. 展开更多
关键词 SUPERALLOYS Rapid solidification Low-cycle fatigue MICROSTRUCTURE
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1.0 T开放式MRI扫描设备实时引导下脑活检 被引量:7
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作者 X.G.He M.Liu +5 位作者 c.liu J.Fang Y.J.Xu L.G.Wang 杨淑娟(译) 赵世华(校) 《国际医学放射学杂志》 北大核心 2019年第2期243-243,共1页
目的评价1.0 T开放式MRI实时引导下脑活检的安全性、可行性及诊断价值。方法86例病人在1.0 T开放式MRI实时引导及MR透视技术下行脑穿刺活检,并回顾性分析其临床资料。
关键词 实时引导 脑活检 MRI 开放式
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Time-Resolved Study of Pseudogap and Superconducting Quasiparticle Dynamics in Ca0.82La0.18Fe1-xNixAs2 被引量:1
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作者 Cong-Ying Jiang Hai-Ying Song +9 位作者 T.Xie c.liu H.Q.Luo S.Z.Zhao Xiu Zhang X.C.Nie Jian-Qiao Meng Yu-Xia Duan H.Y.Liu Shi-Bing Liu 《Chinese Physics Letters》 SCIE CAS CSCD 2020年第6期86-89,共4页
We use femtosecond time-resolved optical reflectivity to study the photoexcited quasiparticle(QP)dynamics in the iron-based 112 type superconducting(SC)samples Ca0.82La0.18Fe1-xNixAs2,with x=0 and 0.024.In the parent ... We use femtosecond time-resolved optical reflectivity to study the photoexcited quasiparticle(QP)dynamics in the iron-based 112 type superconducting(SC)samples Ca0.82La0.18Fe1-xNixAs2,with x=0 and 0.024.In the parent sample,a fast and a slow relaxation emerge at temperatures below the magnetic-structure(MS)transition Tms≈50 K and the SC transition Tc≈33 K,respectively.The latter obviously corresponds to an SC QP dynamics,which is further confirmed in the x=0.024 sample with Tc≈25 K.The former suggests that a partial of photoexcited QP relaxation through a pesudogap(PG)channel,which is absent in the doped x=0.024 sample without the MS transition. 展开更多
关键词 transition. RELAXATION EXCITED
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Influence of single-pass caliber rolling on the microstructural evolution and mechanical properties of Mg–10Gd binary alloy
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作者 H.Yu Z.K.Liu +6 位作者 Y.Liu W.Yu Y.L.Xu c.liu B.A.Jiang S.H.Park K.S.Shin 《Journal of Magnesium and Alloys》 CSCD 2024年第12期5119-5131,共13页
This study investigates the influence of varying rolling reduction on the evolution of microstructure and mechanical properties of Mg–10Gd(in wt%)alloys by caliber rolling(CR).By increasing the rolling reduction from... This study investigates the influence of varying rolling reduction on the evolution of microstructure and mechanical properties of Mg–10Gd(in wt%)alloys by caliber rolling(CR).By increasing the rolling reduction from 45%to 65%,a uniform bimodal structure is obtained in which coarse grains(CGs)larger than 10μm are surrounded by fine grains(FGs).The Mg–Gd alloy subjected to 65%reduction exhibits superior mechanical properties,i.e.yield strength(YS)of~424 MPa,ultimate tensile strength(UTS)of~500 MPa and elongation(El.)of~3.3%.The synergistic improvement in strength and ductility is primarily attributed to the combined effects of low-angle grain boundary(LAGB)strengthening,precipitation strengthening,and the coordinated deformation exhibited by the bimodal structure.In addition,caliber rolling also provides a novel approach for the design of Mg alloys with uniform bimodal structures that exhibit both high strength and ductility. 展开更多
关键词 Mg–Gd alloy Caliber rolling Bimodal microstructure Mechanical properties
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Search for the lepton number violating process J/ψ→K^(+)K^(+)e^(-)e^(-)+c.c.
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作者 M.Ablikim M.N.Achasov +727 位作者 P.Adlarson X.C.Ai R.Aliberti A.Amoroso Q.An Y.Bai O.Bakina Y.Ban H.-R.Bao V.Batozskaya K.Begzsuren N.Berger M.Berlowski M.B.Bertani D.Bettoni F.Bianchi E.Bianco A.Bortone I.Boyko R.A.Briere A.Brueggemann H.Cai M.H.Cai X.Cai A.Calcaterra G.F.Cao N.Cao S.A.Cetin X.Y.Chai J.F.Chang T.T.Chang G.R.Che Y.Z.Che C.H.Chen Chao Chen G.Chen H.S.Chen H.Y.Chen M.L.Chen S.J.Chen S.L.Chen S.M.Chen T.Chen X.R.Chen X.T.Chen X.Y.Chen Y.B.Chen Y.Q.Chen Z.Chen Z.K.Chen J.C.Cheng L.N.Cheng S.K.Choi X.Chu G.Cibinetto F.Cossio J.Cottee-Meldrum H.L.Dai J.P.Dai A.Dbeyssi R.E.de Boer D.Dedovich C.Q.Deng Z.Y.Deng A.Denig I.Denisenko M.Destefanis F.De Mori B.Ding X.X.Ding Y.Ding Y.Ding Y.X.Ding J.Dong L.Y.Dong M.Y.Dong X.Dong M.C.Du S.X.Du S.X.Du X.L.Du Y.Y.Duan Z.H.Duan P.Egorov G.F.Fan J.J.Fan Y.H.Fan J.Fang J.Fang S.S.Fang W.X.Fang Y.Q.Fang R.Farinelli L.Fava F.Feldbauer G.Felici C.Q.Feng J.H.Feng L.Feng Q.X.Feng Y.T.Feng M.Fritsch C.D.Fu J.L.Fu Y.W.Fu H.Gao X.B.Gao Y.Gao Y.N.Gao Y.N.Gao Y.Y.Gao Z.Gao S.Garbolino I.Garzia P.T.Ge Z.W.Ge C.Geng E.M.Gersabeck A.Gilman K.Goetzen J.D.Gong L.Gong W.X.Gong W.Gradl S.Gramigna M.Greco M.H.Gu Y.T.Gu C.Y.Guan A.Q.Guo J.N.Guo L.B.Guo M.J.Guo R.P.Guo X.Guo Y.P.Guo A.Guskov J.Gutierrez K.L.Han T.T.Han F.Hanisch K.D.Hao X.Q.Hao F.A.Harris K.K.He K.L.He F.H.Heinsius C.H.Heinz Y.K.Heng C.Herold P.C.Hong G.Y.Hou X.T.Hou Y.R.Hou Z.L.Hou H.M.Hu J.F.Hu Q.P.Hu S.L.Hu T.Hu Y.Hu Z.M.Hu G.S.Huang K.X.Huang L.Q.Huang P.Huang X.T.Huang Y.P.Huang Y.S.Huang T.Hussain N.Hüsken N.in der Wiesche J.Jackson Q.Ji Q.P.Ji W.Ji X.B.Ji X.L.Ji X.Q.Jia Z.K.Jia D.Jiang H.B.Jiang P.C.Jiang S.J.Jiang X.S.Jiang Y.Jiang J.B.Jiao J.K.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing X.M.Jing T.Johansson S.Kabana N.Kalantar-Nayestanaki X.L.Kang X.S.Kang M.Kavatsyuk B.C.Ke V.Khachatryan A.Khoukaz O.B.Kolcu B.Kopf M.Kuessner X.Kui N.Kumar A.Kupsc W.Kühn Q.Lan W.N.Lan T.T.Lei M.Lellmann T.Lenz C.Li C.Li C.H.Li C.K.Li D.M.Li F.Li G.Li H.B.Li H.J.Li H.N.Li Hui Li J.R.Li J.S.Li J.W.Li K.Li K.L.Li K.L.Li L.J.Li Lei Li M.H.Li M.R.Li P.L.Li P.R.Li Q.M.Li Q.X.Li R.Li S.X.Li T.Li T.Y.Li W.D.Li W.G.Li X.Li X.H.Li X.L.Li X.Y.Li X.Z.Li Y.Li Y.G.Li Y.P.Li Z.J.Li Z.X.Li Z.Y.Li C.Liang H.Liang Y.F.Liang Y.T.Liang G.R.Liao L.B.Liao M.H.Liao Y.P.Liao J.Libby A.Limphirat C.C.Lin D.X.Lin L.Q.Lin T.Lin B.J.Liu B.X.Liu c.liu C.X.Liu F.Liu F.H.Liu Feng Liu G.M.Liu H.Liu H.B.Liu H.H.Liu H.M.Liu Huihui Liu J.B.Liu J.J.Liu K.Liu K.Liu K.Y.Liu Ke Liu L.c.liu Lu Liu M.H.Liu P.L.Liu Q.Liu S.B.Liu T.Liu W.K.Liu W.M.Liu W.T.Liu X.Liu X.Liu X.K.Liu X.L.Liu X.Y.Liu Y.Liu Y.Liu Y.B.Liu Z.A.Liu Z.D.Liu Z.Q.Liu X.C.Lou H.J.Lu J.G.Lu X.L.Lu Y.Lu Y.H.Lu Y.P.Lu Z.H.Lu C.L.Luo J.R.Luo J.S.Luo M.X.Luo T.Luo X.L.Luo Z.Y.Lv X.R.Lyu Y.F.Lyu Y.H.Lyu F.C.Ma H.L.Ma Heng Ma J.L.Ma L.L.Ma L.R.Ma Q.M.Ma R.Q.Ma R.Y.Ma T.Ma X.T.Ma X.Y.Ma Y.M.Ma F.E.Maas I.MacKay M.Maggiora S.Malde Q.A.Malik H.X.Mao Y.J.Mao Z.P.Mao S.Marcello A.Marshall F.M.Melendi Y.H.Meng Z.X.Meng G.Mezzadri H.Miao T.J.Min R.E.Mitchell X.H.Mo B.Moses N.Yu.Muchnoi J.Muskalla Y.Nefedov F.Nerling Z.Ning S.Nisar Q.L.Niu W.D.Niu Y.Niu C.Normand S.L.Olsen Q.Ouyang S.Pacetti X.Pan Y.Pan A.Pathak Y.P.Pei M.Pelizaeus H.P.Peng X.J.Peng Y.Y.Peng K.Peters K.Petridis J.L.Ping R.G.Ping S.Plura V.Prasad F.Z.Qi H.R.Qi M.Qi S.Qian W.B.Qian C.F.Qiao J.H.Qiao J.J.Qin J.L.Qin L.Q.Qin L.Y.Qin P.B.Qin X.P.Qin X.S.Qin Z.H.Qin J.F.Qiu Z.H.Qu J.Rademacker C.F.Redmer A.Rivetti M.Rolo G.Rong S.S.Rong F.Rosini Ch.Rosner M.Q.Ruan N.Salone A.Sarantsev Y.Schelhaas K.Schoenning M.Scodeggio K.Y.Shan W.Shan X.Y.Shan Z.J.Shang J.F.Shangguan L.G.Shao M.Shao C.P.Shen H.F.Shen W.H.Shen X.Y.Shen B.A.Shi H.Shi J.L.Shi J.Y.Shi S.Y.Shi X.Shi H.L.Song J.J.Song T.Z.Song W.M.Song Y.J.Song Y.X.Song Zirong Song S.Sosio S.Spataro F.Stieler S.S Su Y.J.Su G.B.Sun G.X.Sun H.Sun H.K.Sun J.F.Sun K.Sun L.Sun R.Sun S.S.Sun T.Sun Y.C.Sun Y.H.Sun Y.J.Sun Y.Z.Sun Z.Q.Sun Z.T.Sun C.J.Tang G.Y.Tang J.Tang J.J.Tang L.F.Tang Y.A.Tang L.Y.Tao M.Tat J.X.Teng J.Y.Tian W.H.Tian Y.Tian Z.F.Tian I.Uman B.Wang B.Wang Bo Wang C.Wang C.Wang Cong Wang D.Y.Wang H.J.Wang J.J.Wang J.P.Wang K.Wang L.L.Wang L.W.Wang M.Wang M.Wang N.Y.Wang S.Wang S.Wang T.Wang T.J.Wang W.Wang W.Wang W.P.Wang X.Wang X.F.Wang X.J.Wang X.L.Wang X.N.Wang Y.Wang Y.D.Wang Y.F.Wang Y.H.Wang Y.J.Wang Y.L.Wang Y.N.Wang Y.N.Wang Y.Q.Wang Yaqian Wang Yi Wang Yuan Wang Z.Wang Z.Wang Z.L.Wang Z.L.Wang Z.Q.Wang Z.Y.Wang Ziyi Wang D.Wei D.H.Wei H.R.Wei F.Weidner S.P.Wen Y.R.Wen U.Wiedner G.Wilkinson M.Wolke C.Wu J.F.Wu L.H.Wu L.J.Wu L.J.Wu Lianjie Wu S.G.Wu S.M.Wu X.Wu X.H.Wu Y.J.Wu Z.Wu L.Xia X.M.Xian B.H.Xiang D.Xiao G.Y.Xiao H.Xiao Y.L.Xiao Z.J.Xiao C.Xie K.J.Xie Y.Xie Y.G.Xie Y.H.Xie Z.P.Xie T.Y.Xing C.F.Xu C.J.Xu G.F.Xu H.Y.Xu M.Xu Q.J.Xu Q.N.Xu T.D.Xu W.Xu W.L.Xu X.P.Xu Y.Xu Y.C.Xu Z.S.Xu F.Yan F.Yan H.Y.Yan L.Yan W.B.Yan W.C.Yan W.H.Yan W.P.Yan X.Q.Yan H.J.Yang H.L.Yang H.X.Yang J.H.Yang R.J.Yang Y.Yang Y.H.Yang Y.Q.Yang Y.X.Yang Y.Z.Yang Z.P.Yao M.Ye M.H.Ye Z.J.Ye Junhao Yin Z.Y.You B.X.Yu C.X.Yu G.Yu J.S.Yu L.W.Yu M.C.Yu T.Yu X.D.Yu Y.C.Yu C.Z.Yuan H.Yuan J.Yuan J.Yuan L.Yuan M.K.Yuan S.C.Yuan S.H.Yuan X.Q.Yuan Y.Yuan Z.Y.Yuan C.X.Yue Ying Yue A.A.Zafar F.R.Zeng S.H.Zeng X.Zeng Y.J.Zeng Y.J.Zeng Y.C.Zhai Y.H.Zhan A.Q.Zhang B.L.Zhang B.X.Zhang D.H.Zhang G.Y.Zhang G.Y.Zhang H.Zhang H.Zhang H.C.Zhang H.H.Zhang H.Q.Zhang H.R.Zhang H.Y.Zhang J.Zhang J.J.Zhang J.L.Zhang J.Q.Zhang J.S.Zhang J.W.Zhang J.X.Zhang J.Y.Zhang J.Z.Zhang Jianyu Zhang L.M.Zhang Lei Zhang N.Zhang P.Zhang Q.Zhang Q.Y.Zhang R.Y.Zhang S.H.Zhang Shulei Zhang X.M.Zhang X.Y Zhang X.Y.Zhang Y.Zhang Y.Zhang Y.T.Zhang Y.H.Zhang Y.M.Zhang Y.P.Zhang Z.D.Zhang Z.H.Zhang Z.L.Zhang Z.L.Zhang Z.X.Zhang Z.Y.Zhang Z.Y.Zhang Z.Z.Zhang Zh.Zh.Zhang G.Zhao J.Y.Zhao J.Z.Zhao L.Zhao L.Zhao M.G.Zhao N.Zhao R.P.Zhao S.J.Zhao Y.B.Zhao Y.L.Zhao Y.X.Zhao Z.G.Zhao A.Zhemchugov B.Zheng B.M.Zheng J.P.Zheng W.J.Zheng X.R.Zheng Y.H.Zheng B.Zhong C.Zhong H.Zhou J.Q.Zhou S.Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou Y.X.Zhou Y.Z.Zhou A.N.Zhu J.Zhu K.Zhu K.J.Zhu K.S.Zhu L.Zhu L.X.Zhu S.H.Zhu T.J.Zhu W.D.Zhu W.D.Zhu W.J.Zhu W.Z.Zhu Y.C.Zhu Z.A.Zhu X.Y.Zhuang J.H.Zou J.Zu 《Chinese Physics C》 2026年第1期120-130,共11页
Based on(10087±44)×10^(6) J/ψevents collected with the BESⅢdetector,we search for the lepton number violating decay J/ψ→K^(+)K^(+)e^(-)e^(-)+c.c.for the first time.The upper limit on the branching fracti... Based on(10087±44)×10^(6) J/ψevents collected with the BESⅢdetector,we search for the lepton number violating decay J/ψ→K^(+)K^(+)e^(-)e^(-)+c.c.for the first time.The upper limit on the branching fraction of this decay is set to 2.1×10^(-9)at the 90%confidence level with a frequentist method.This is the first search for J/ψdecays with a lepton number change by two,offering valuable insights into the underlying physical processes. 展开更多
关键词 Lepton number violation matter anti-matter asymmetry neutrinoless double beta decay
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Observation of theγ-ray emission from W43 with LHAASO
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作者 Zhen Cao F.A.haronian +296 位作者 Axikegu Y.X.Bai Y.W.Bao D.Bastieri X.J.Bi Y.J.Bi W.Bian A.V.Bukevich Q.Cao W.Y.Cao Zhe Cao J.Chang J.F.Chang A.M.Chen E.S.Chen H.X.Chen Liang Chen Lin Chen Long Chen M.J.Chen M.L.Chen Q.H.Chen S.Chen S.H.Chen S.Z.Chen T.L.Chen Y.Chen N.Cheng Y.D.Cheng M.C.Chu M.Y.Cui S.W.Cui X.H.Cui Y.D.Cui B.Z.Dai H.L.Dai Z.G.Dai Danzengluobu X.Q.Dong K.K.Duan J.H.Fan Y.Z.Fan J.Fang J.H.Fang K.Fang C.F.Feng H.Feng L.Feng S.H.Feng X.T.Feng Y.Feng Y.L.Feng S.Gabici B.Gao C.D.Gao Q.Gao W.Gao W.K.Gao M.M.Ge T.T.Ge L.S.Geng G.Giacinti G.H.Gong Q.B.Gou M.H.Gu F.L.Guo J.Guo X.L.Guo Y.Q.Guo Y.Y.Guo Y.A.Han O.A.Hannuksela M.Hasan H.H.He H.N.He J.Y.He Y.He Y.K.Hor B.W.Hou C.Hou X.Hou H.B.Hu Q.Hu S.C.Hu C.Huang D.H.Huang T.Q.Huang W.J.Huang X.T.Huang X.Y.Huang Y.Huang Y.Y.Huang X.L.Ji H.Y.Jia K.Jia H.B.Jiang K.Jiang X.W.Jiang Z.J.Jiang M.Jin M.M.Kang I.Karpikov D.K.hangulyan D.Kuleshov K.Kurinov B.B.Li C.M.Li Cheng Li Cong Li D.Li F.Li H.B.Li H.C.Li Jian Li Jie Li K.Li S.D.Li W.L.Li W.L.Li X.R.Li Xin Li Y.Z.Li Zhe Li Zhuo Li E.W.Liang Y.F.Liang S.J.Lin B.Liu c.liu D.Liu D.B.Liu H.Liu H.D.Liu J.Liu J.L.Liu M.Y.Liu R.Y.Liu S.M.Liu W.Liu Y.Liu Y.N.Liu Q.Luo Y.Luo H.K.Lv B.Q.Ma L.L.Ma X.H.Ma J.R.Mao Z.Min W.Mitthumsiri H.J.Mu Y.C.Nan A.Neronov K.C.Y.Ng L.J.Ou P.Pattarakijwanich Z.Y.Pei J.C.Qi M.Y.Qi B.Q.Qiao J.J.Qin A.Raza D.Ruffolo A.Saiz´ M.Saeed D.Semikoz L.Shao O.Shchegolev X.D.Sheng F.W.Shu H.C.Song Yu V.Stenkin V.Stepanov Y.Su D.X.Sun Q.N.Sun X.N.Sun Z.B.Sun J.Takata P.H.T.Tam Q.W.Tang R.Tang Z.B.Tang W.W.Tian L.H.Wan C.Wang C.B.Wang G.W.Wang H.G.Wang H.H.Wang J.C.Wang Kai Wang Kai Wang L.P.Wang L.Y.Wang P.H.Wang R.Wang W.Wang X.G.Wang X.Y.Wang Y.Wang Y.D.Wang Y.J.Wang Z.H.Wang Z.X.Wang Zhen Wang Zheng Wang D.M.Wei J.J.Wei Y.J.Wei T.Wen C.Y.Wu H.R.Wu Q.W.Wu S.Wu X.F.Wu Y.S.Wu S.Q.Xi J.Xia G.M.Xiang D.X.Xiao G.Xiao Y.L.Xin Y.Xing D.R.Xiong Z.Xiong D.L.Xu R.F.Xu R.X.Xu W.L.Xu L.Xue D.H.Yan J.Z.Yan T.Yan C.W.Yang C.Y.Yang F.Yang F.F.Yang L.L.Yang M.J.Yang R.Z.Yang W.X.Yang Y.H.Yao Z.G.Yao L.Q.Yin N.Yin X.H.You Z.Y.You Y.H.Yu Q.Yuan H.Yue H.D.Zeng T.X.Zeng W.Zeng M.Zha B.B.Zhang F.Zhang H.Zhang H.M.Zhang H.Y.Zhang J.L.Zhang Li Zhang P.F.Zhang P.P.Zhang R.Zhang S.B.Zhang S.R.Zhang S.S.Zhang X.Zhang X.P.Zhang Y.F.Zhang Yi Zhang Yong Zhang B.Zhao J.Zhao L.Zhao L.Z.Zhao S.P.Zhao X.H.Zhao F.Zheng W.J.Zhong B.Zhou H.Zhou J.N.Zhou M.Zhou P.Zhou R.Zhou X.X.Zhou X.X.Zhou B.Y.Zhu C.G.Zhu F.R.Zhu H.Zhu K.J.Zhu Y.C.Zou X.Zuo The LHAASO Collaboration 《Science China(Physics,Mechanics & Astronomy)》 2025年第7期2-12,共11页
In this paper,we report the detection of the very-high-energy(VHE,100 GeV<E<100 TeV)and ultra-high-energy(UHE,E>100 TeV)y-ray emissions from the direction of the young star-forming region W43,observed by the ... In this paper,we report the detection of the very-high-energy(VHE,100 GeV<E<100 TeV)and ultra-high-energy(UHE,E>100 TeV)y-ray emissions from the direction of the young star-forming region W43,observed by the Large High Altitude Air Shower Observation(LHAASO).The extendedγ-ray source was detected with a significance of~16σby KM2A and~17σby WCDA,respectively.The angular extension of this y-ray source is about 0.5 degrees,corresponding to a physical size of about 50pc.We discuss the origin of theγ-ray emission and possible cosmic ray acceleration in the W43 region using multi-wavelength data.Our findings suggest that W43 is likely another young star cluster capable of accelerating cosmic rays(CRs)to at least several hundred TeV. 展开更多
关键词 large high altitude air shower observation lhaaso gamma ray emission cosmic ray acceleration multi wavelength data ultra high energy gamma rays W star forming region very high energy gamma rays
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LHAASO detection of very-high-energyγ-ray emission surrounding PSR J0248+6021
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作者 Zhen Cao F.A.haronian +296 位作者 Axikegu Y.X.Bai Y.W.Bao D.Bastieri X.J.Bi Y.J.Bi W.Bian A.V.Bukevich Q.Cao W.Y.Cao Zhe Cao J.Chang J.F.Chang A.M.Chen E.S.Chen H.X.Chen Liang Chen Lin Chen Long Chen M.J.Chen M.L.Chen Q.H.Chen S.Chen S.H.Chen S.Z.Chen T.L.Chen Y.Chen N.Cheng Y.D.Cheng M.C.Chu M.Y.Cui S.W.Cui X.H.Cui Y.D.Cui B.Z.Dai H.L.Dai Z.G.Dai Danzengluobu X.Q.Dong K.K.Duan J.H.Fan Y.Z.Fan J.Fang J.H.Fang K.Fang C.F.Feng H.Feng L.Feng S.H.Feng X.T.Feng Y.Feng Y.L.Feng S.Gabici B.Gao C.D.Gao Q.Gao W.Gao W.K.Gao M.M.Ge T.T.Ge L.S.Geng G.Giacinti G.H.Gong Q.B.Gou M.H.Gu F.L.Guo J.Guo X.L.Guo Y.Q.Guo Y.Y.Guo Y.A.Han O.A.Hannuksela M.Hasan H.H.He H.N.He J.Y.He Y.He Y.K.Hor B.W.Hou C.Hou X.Hou H.B.Hu Q.Hu S.C.Hu C.Huang D.H.Huang T.Q.Huang W.J.Huang X.T.Huang X.Y.Huang Y.Huang Y.Y.Huang X.L.Ji H.Y.Jia K.Jia H.B.Jiang K.Jiang X.W.Jiang Z.J.Jiang M.Jin M.M.Kang I.Karpikov D.K.hangulyan D.Kuleshov K.Kurinov B.B.Li C.M.Li Cheng Li Cong Li D.Li F.Li H.B.Li H.C.Li Jian Li Jie Li K.Li S.D.Li W.L.Li W.L.Li X.R.Li Xin Li Y.Z.Li Zhe Li Zhuo Li E.W.Liang Y.F.Liang S.J.Lin B.Liu c.liu D.Liu D.B.Liu H.Liu H.D.Liu J.Liu J.L.Liu M.Y.Liu R.Y.Liu S.M.Liu W.Liu Y.Liu Y.N.Liu Q.Luo Y.Luo H.K.Lv B.Q.Ma L.L.Ma X.H.Ma J.R.Mao Z.Min W.Mitthumsiri H.J.Mu Y.C.Nan A.Neronov K.C.Y.Ng L.J.Ou P.Pattarakijwanich Z.Y.Pei J.C.Qi M.Y.Qi B.Q.Qiao J.J.Qin A.Raza D.Ruffolo A.Saiz´ M.Saeed D.Semikoz L.Shao O.Shchegolev X.D.Sheng F.W.Shu H.C.Song Yu V.Stenkin V.Stepanov Y.Su D.X.Sun Q.N.Sun X.N.Sun Z.B.Sun J.Takata P.H.T.Tam Q.W.Tang R.Tang Z.B.Tang W.W.Tian L.H.Wan C.Wang C.B.Wang G.W.Wang H.G.Wang H.H.Wang J.C.Wang Kai Wang Kai Wang L.P.Wang L.Y.Wang P.H.Wang R.Wang W.Wang X.G.Wang X.Y.Wang Y.Wang Y.D.Wang Y.J.Wang Z.H.Wang Z.X.Wang Zhen Wang Zheng Wang D.M.Wei J.J.Wei Y.J.Wei T.Wen C.Y.Wu H.R.Wu Q.W.Wu S.Wu X.F.Wu Y.S.Wu S.Q.Xi J.Xia G.M.Xiang D.X.Xiao G.Xiao Y.L.Xin Y.Xing D.R.Xiong Z.Xiong D.L.Xu R.F.Xu R.X.Xu W.L.Xu L.Xue D.H.Yan J.Z.Yan T.Yan C.W.Yang C.Y.Yang F.Yang F.F.Yang L.L.Yang M.J.Yang R.Z.Yang W.X.Yang Y.H.Yao Z.G.Yao L.Q.Yin N.Yin X.H.You Z.Y.You Y.H.Yu Q.Yuan H.Yue H.D.Zeng T.X.Zeng W.Zeng M.Zha B.B.Zhang F.Zhang H.Zhang H.M.Zhang H.Y.Zhang J.L.Zhang Li Zhang P.F.Zhang P.P.Zhang R.Zhang S.B.Zhang S.R.Zhang S.S.Zhang X.Zhang X.P.Zhang Y.F.Zhang Yi Zhang Yong Zhang B.Zhao J.Zhao L.Zhao L.Z.Zhao S.P.Zhao X.H.Zhao F.Zheng W.J.Zhong B.Zhou H.Zhou J.N.Zhou M.Zhou P.Zhou R.Zhou X.X.Zhou X.X.Zhou B.Y.Zhu C.G.Zhu F.R.Zhu H.Zhu K.J.Zhu Y.C.Zou X.Zuo The LHAASO Collaboration 《Science China(Physics,Mechanics & Astronomy)》 2025年第7期27-37,共11页
We report the detection of an extended very-high-energy(VHE)γ-ray source coincident with the location of middle-aged(62.4 kyr)pulsar PSR J0248+6021,by using the LHAASO-WCDA data of live 796 d and LHAASO-KM2A data of ... We report the detection of an extended very-high-energy(VHE)γ-ray source coincident with the location of middle-aged(62.4 kyr)pulsar PSR J0248+6021,by using the LHAASO-WCDA data of live 796 d and LHAASO-KM2A data of live 1216d.A significant excess of y-ray induced showers is observed both by WCDA in energy bands of 1-25 TeV and KM2A in energy bands of>25 TeV with 7.3σand 13.5σ,respectively.The best-fit position derived through WCDA data is R.A.=42.06°±0.12°and Dec.=60.24°±0.13°with an extension of 0.69°±0.15°and that of the KM2A data is R.A.=42.29°±0.13°and Dec.=60.38°±0.07°with an extension of 0.37°±0.07°.No clear extended multiwavelength counterpart of this LHAASO source has been found from the radio band to the GeV band.The most plausible explanation of the VHEγ-ray emission is the inverse Compton process of highly relativistic electrons and positrons injected by the pulsar.These electrons/positrons are hypothesized to be either confined within the pulsar wind nebula or to have already escaped into the interstellar medium,forming a pulsar halo. 展开更多
关键词 γ-rays PULSARS individual PSR J0248+6021 interstellar medium(ISM) NEBULAE
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Study of ultra-high-energy gamma-ray source 1LHAASO J0056+6346u and its possible origins
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作者 Zhen Cao F.A.haronian +296 位作者 Axikegu Y.X.Bai Y.W.Bao D.Bastieri X.J.Bi Y.J.Bi W.Bian A.V.Bukevich Q.Cao W.Y.Cao Zhe Cao J.Chang J.F.Chang A.M.Chen E.S.Chen H.X.Chen Liang Chen Lin Chen Long Chen M.J.Chen M.L.Chen Q.H.Chen S.Chen S.H.Chen S.Z.Chen T.L.Chen Y.Chen N.Cheng Y.D.Cheng M.C.Chu M.Y.Cui S.W.Cui X.H.Cui Y.D.Cui B.Z.Dai H.L.Dai Z.G.Dai Danzengluobu X.Q.Dong K.K.Duan J.H.Fan Y.Z.Fan J.Fang J.H.Fang K.Fang C.F.Feng H.Feng L.Feng S.H.Feng X.T.Feng Y.Feng Y.L.Feng S.Gabici B.Gao C.D.Gao Q.Gao W.Gao W.K.Gao M.M.Ge T.T.Ge L.S.Geng G.Giacinti G.H.Gong Q.B.Gou M.H.Gu F.L.Guo J.Guo X.L.Guo Y.Q.Guo Y.Y.Guo Y.A.Han O.A.Hannuksela M.Hasan H.H.He H.N.He J.Y.He Y.He Y.K.Hor B.W.Hou C.Hou X.Hou H.B.Hu Q.Hu S.C.Hu C.Huang D.H.Huang T.Q.Huang W.J.Huang X.T.Huang X.Y.Huang Y.Huang Y.Y.Huang X.L.Ji H.Y.Jia K.Jia H.B.Jiang K.Jiang X.W.Jiang Z.J.Jiang M.Jin M.M.Kang I.Karpikov D.K.hangulyan D.Kuleshov K.Kurinov B.B.Li C.M.Li Cheng Li Cong Li D.Li F.Li H.B.Li H.C.Li Jian Li Jie Li K.Li S.D.Li W.L.Li W.L.Li X.R.Li Xin Li Y.Z.Li Zhe Li Zhuo Li E.W.Liang Y.F.Liang S.J.Lin B.Liu c.liu D.Liu D.B.Liu H.Liu H.D.Liu J.Liu J.L.Liu M.Y.Liu R.Y.Liu S.M.Liu W.Liu Y.Liu Y.N.Liu Q.Luo Y.Luo H.K.Lv B.Q.Ma L.L.Ma X.H.Ma J.R.Mao Z.Min W.Mitthumsiri H.J.Mu Y.C.Nan A.Neronov K.C.Y.Ng L.J.Ou P.Pattarakijwanich Z.Y.Pei J.C.Qi M.Y.Qi B.Q.Qiao J.J.Qin A.Raza D.Ruffolo A.Saiz´ M.Saeed D.Semikoz L.Shao O.Shchegolev X.D.Sheng F.W.Shu H.C.Song Yu V.Stenkin V.Stepanov Y.Su D.X.Sun Q.N.Sun X.N.Sun Z.B.Sun J.Takata P.H.T.Tam Q.W.Tang R.Tang Z.B.Tang W.W.Tian L.H.Wan C.Wang C.B.Wang G.W.Wang H.G.Wang H.H.Wang J.C.Wang Kai Wang Kai Wang L.P.Wang L.Y.Wang P.H.Wang R.Wang W.Wang X.G.Wang X.Y.Wang Y.Wang Y.D.Wang Y.J.Wang Z.H.Wang Z.X.Wang Zhen Wang Zheng Wang D.M.Wei J.J.Wei Y.J.Wei T.Wen C.Y.Wu H.R.Wu Q.W.Wu S.Wu X.F.Wu Y.S.Wu S.Q.Xi J.Xia G.M.Xiang D.X.Xiao G.Xiao Y.L.Xin Y.Xing D.R.Xiong Z.Xiong D.L.Xu R.F.Xu R.X.Xu W.L.Xu L.Xue D.H.Yan J.Z.Yan T.Yan C.W.Yang C.Y.Yang F.Yang F.F.Yang L.L.Yang M.J.Yang R.Z.Yang W.X.Yang Y.H.Yao Z.G.Yao L.Q.Yin N.Yin X.H.You Z.Y.You Y.H.Yu Q.Yuan H.Yue H.D.Zeng T.X.Zeng W.Zeng M.Zha B.B.Zhang F.Zhang H.Zhang H.M.Zhang H.Y.Zhang J.L.Zhang Li Zhang P.F.Zhang P.P.Zhang R.Zhang S.B.Zhang S.R.Zhang S.S.Zhang X.Zhang X.P.Zhang Y.F.Zhang Yi Zhang Yong Zhang B.Zhao J.Zhao L.Zhao L.Z.Zhao S.P.Zhao X.H.Zhao F.Zheng W.J.Zhong B.Zhou H.Zhou J.N.Zhou M.Zhou P.Zhou R.Zhou X.X.Zhou X.X.Zhou B.Y.Zhu C.G.Zhu F.R.Zhu H.Zhu K.J.Zhu Y.C.Zou X.Zuo The LHAASO Collaboration 《Science China(Physics,Mechanics & Astronomy)》 2025年第7期38-50,共13页
We report a dedicated study of the newly discovered extended UHEγ-ray source 1LHAASO J0056+6346u.Analyzing 979 d of LHAASO-WCDA data and 1389 d of LHAASO-KM2A data,we observed a significant excess ofγ-ray events wit... We report a dedicated study of the newly discovered extended UHEγ-ray source 1LHAASO J0056+6346u.Analyzing 979 d of LHAASO-WCDA data and 1389 d of LHAASO-KM2A data,we observed a significant excess ofγ-ray events with both WCDA and KM2A.Assuming a point power-law source with a fixed spectral index,the significance maps reveal excesses of 12.65σ,22.18σ,and 10.24σin the energy ranges of 1-25,25-100,and>100 TeV,respectively.We use a 3D likelihood algorithm to derive the morphological and spectral parameters,and the source is detected with significances of 13.72σby WCDA and 25.27σby KM2A.The best-fit positions derived from WCDA and KM2A data are(R.A.=13.96°±0.09°,Decl.=63.92°±0.05°)and(R.A.=14.00°±0.05°,Decl.=63.79°±0.02°),respectively.The angular size(r_(39))of 1LHAASO J0056+6346u is 0.34°±0.04°at 1-25 TeV and 0.24°±0.02°at>25 TeV.The differential flux of this UHEγ-ray source can be described by an exponential cutoff power-law function:(2.67±0.25)×10^(-15)(E/20 TeV)^((-1.97±0.10))e^(-E/(55.1±7.2)TeV)TeV^(-1)cm^(-2)s^(-1).To explore potential sources ofγ-ray emission,we investigated the gas distribution around 1LHAASO J0056+6346u.1LHAASO J0056+6346u is likely to be a TeV PWN powered by an unknown pulsar,which would naturally explain both its spatial and spectral properties.Another explanation is that this UHEγ-ray source might be associated with gas content illuminated by a nearby CR accelerator,possibly the SNR candidate G124.0+1.4. 展开更多
关键词 gamma rays cosmic rays supernova remnant young massive cluster pulsar
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Precise measurement of the χ_(c 0) resonance parameters and branching fractions ofχ_(c 0,c 2)→π^(+)π^(−)/K^(+)K^(−)
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作者 M.Ablikim M.N.Achasov +669 位作者 P.Adlarson O.Afedulidis X.C.Ai R.Aliberti A.Amoroso Y.Bai O.Bakina I.Balossino Y.Ban H.-R.Bao V.Batozskaya K.Begzsuren N.Berger M.Berlowski M.Bertani D.Bettoni F.Bianchi E.Bianco A.Bortone I.Boyko R.A.Briere A.Brueggemann H.Cai X.Cai A.Calcaterra G.F.Cao N.Cao S.A.Cetin X.Y.Chai J.F.Chang G.R.Che Y.Z.Che G.Chelkov C.Chen C.H.Chen Chao Chen G.Chen H.S.Chen H.Y.Chen M.L.Chen S.J.Chen S.L.Chen S.M.Chen T.Chen X.R.Chen X.T.Chen Y.B.Chen Y.Q.Chen Z.J.Chen Z.Y.Chen S.K.Choi G.Cibinetto F.Cossio J.J.Cui H.L.Dai J.P.Dai A.Dbeyssi R.E.de Boer D.Dedovich C.Q.Deng Z.Y.Deng A.Denig I.Denisenko M.Destefanis F.De Mori B.Ding X.X.Ding Y.Ding Y.Ding J.Dong L.Y.Dong M.Y.Dong X.Dong M.C.Du S.X.Du Y.Y.Duan Z.H.Duan P.Egorov Y.H.Fan J.Fang J.Fang S.S.Fang W.X.Fang Y.Fang Y.Q.Fang R.Farinelli L.Fava F.Feldbauer G.Felici C.Q.Feng J.H.Feng Y.T.Feng M.Fritsch C.D.Fu J.L.Fu Y.W.Fu H.Gao X.B.Gao Y.N.Gao Yang Gao S.Garbolino I.Garzia L.Ge P.T.Ge Z.W.Ge C.Geng E.M.Gersabeck A.Gilman K.Goetzen L.Gong W.X.Gong W.Gradl S.Gramigna M.Greco M.H.Gu Y.T.Gu C.Y.Guan A.Q.Guo L.B.Guo M.J.Guo R.P.Guo Y.P.Guo A.Guskov J.Gutierrez K.L.Han T.T.Han F.Hanisch X.Q.Hao F.A.Harris K.K.He K.L.He F.H.Heinsius C.H.Heinz Y.K.Heng C.Herold T.Holtmann P.C.Hong G.Y.Hou X.T.Hou Y.R.Hou Z.L.Hou B.Y.Hu H.M.Hu J.F.Hu Q.P.Hu S.L.Hu T.Hu Y.Hu G.S.Huang K.X.Huang L.Q.Huang X.T.Huang Y.P.Huang Y.S.Huang T.Hussain F.Hölzken N.Hüsken N.in der Wiesche J.Jackson S.Janchiv J.H.Jeong Q.Ji Q.P.Ji W.Ji X.B.Ji X.L.Ji Y.Y.Ji X.Q.Jia Z.K.Jia D.Jiang H.B.Jiang P.C.Jiang S.S.Jiang T.J.Jiang X.S.Jiang Y.Jiang J.B.Jiao J.K.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing X.M.Jing T.Johansson S.Kabana N.Kalantar-Nayestanaki X.L.Kang X.S.Kang M.Kavatsyuk B.C.Ke V.Khachatryan A.Khoukaz R.Kiuchi O.B.Kolcu B.Kopf M.Kuessner X.Kui N.Kumar A.Kupsc W.Kühn L.Lavezzi T.T.Lei Z.H.Lei M.Lellmann T.Lenz C.Li C.Li C.H.Li Cheng Li D.M.Li F.Li G.Li H.B.Li H.J.Li H.N.Li Hui Li J.R.Li J.S.Li K.Li K.L.Li L.J.Li L.K.Li Lei Li M.H.Li P.R.Li Q.M.Li Q.X.Li R.Li S.X.Li T.Li T.Y.Li W.D.Li W.G.Li X.Li X.H.Li X.L.Li X.Y.Li X.Z.Li Y.G.Li Z.J.Li Z.Y.Li C.Liang H.Liang H.Liang Y.F.Liang Y.T.Liang G.R.Liao Y.P.Liao J.Libby A.Limphirat C.C.Lin C.X.Lin D.X.Lin T.Lin B.J.Liu B.X.Liu c.liu C.X.Liu F.Liu F.H.Liu Feng Liu G.M.Liu H.Liu H.B.Liu H.H.Liu H.M.Liu Huihui Liu J.B.Liu J.Y.Liu K.Liu K.Y.Liu Ke Liu L.Liu L.c.liu Lu Liu M.H.Liu P.L.Liu Q.Liu S.B.Liu T.Liu W.K.Liu W.M.Liu X.Liu X.Liu Y.Liu Y.Liu Y.B.Liu Z.A.Liu Z.D.Liu Z.Q.Liu X.C.Lou F.X.Lu H.J.Lu J.G.Lu X.L.Lu Y.Lu Y.P.Lu Z.H.Lu C.L.Luo J.R.Luo M.X.Luo T.Luo X.L.Luo X.R.Lyu Y.F.Lyu F.C.Ma H.Ma H.L.Ma J.L.Ma L.L.Ma L.R.Ma M.M.Ma Q.M.Ma R.Q.Ma T.Ma X.T.Ma X.Y.Ma Y.M.Ma F.E.Maas I.MacKay M.Maggiora S.Malde Y.J.Mao Z.P.Mao S.Marcello Z.X.Meng J.G.Messchendorp G.Mezzadri H.Miao T.J.Min R.E.Mitchell X.H.Mo B.Moses N.Yu.Muchnoi J.Muskalla Y.Nefedov F.Nerling L.S.Nie I.B.Nikolaev Z.Ning S.Nisar Q.L.Niu W.D.Niu Y.Niu S.L.Olsen S.L.Olsen Q.Ouyang S.Pacetti X.Pan Y.Pan A.Pathak Y.P.Pei M.Pelizaeus H.P.Peng Y.Y.Peng K.Peters J.L.Ping R.G.Ping S.Plura V.Prasad F.Z.Qi H.Qi H.R.Qi M.Qi T.Y.Qi S.Qian W.B.Qian C.F.Qiao X.K.Qiao J.J.Qin L.Q.Qin L.Y.Qin X.P.Qin X.S.Qin Z.H.Qin J.F.Qiu Z.H.Qu C.F.Redmer K.J.Ren A.Rivetti M.Rolo G.Rong Ch.Rosner M.Q.Ruan S.N.Ruan N.Salone A.Sarantsev Y.Schelhaas K.Schoenning M.Scodeggio K.Y.Shan W.Shan X.Y.Shan Z.J.Shang J.F.Shangguan L.G.Shao M.Shao C.P.Shen H.F.Shen W.H.Shen X.Y.Shen B.A.Shi H.Shi J.L.Shi J.Y.Shi Q.Q.Shi S.Y.Shi X.Shi J.J.Song T.Z.Song W.M.Song Y.J.Song Y.X.Song S.Sosio S.Spataro F.Stieler S.S Su Y.J.Su G.B.Sun G.X.Sun H.Sun H.K.Sun J.F.Sun K.Sun L.Sun S.S.Sun T.Sun W.Y.Sun Y.Sun Y.J.Sun Y.Z.Sun Z.Q.Sun Z.T.Sun C.J.Tang G.Y.Tang J.Tang J.J.Tang Y.A.Tang L.Y.Tao Q.T.Tao M.Tat J.X.Teng V.Thoren W.H.Tian Y.Tian Z.F.Tian I.Uman Y.Wan S.J.Wang B.Wang B.L.Wang Bo Wang D.Y.Wang F.Wang H.J.Wang J.J.Wang J.P.Wang K.Wang L.L.Wang M.Wang N.Y.Wang S.Wang S.Wang T.Wang T.J.Wang W.Wang W.Wang W.P.Wang X.Wang X.F.Wang X.J.Wang X.L.Wang X.N.Wang Y.Wang Y.D.Wang Y.F.Wang Y.H.Wang Y.L.Wang Y.N.Wang Y.Q.Wang Yaqian Wang Yi Wang Z.Wang Z.L.Wang Z.Y.Wang Ziyi Wang D.H.Wei F.Weidner S.P.Wen Y.R.Wen U.Wiedner G.Wilkinson M.Wolke L.Wollenberg C.Wu J.F.Wu L.H.Wu L.J.Wu X.Wu X.H.Wu Y.Wu Y.H.Wu Y.J.Wu Z.Wu L.Xia X.M.Xian B.H.Xiang T.Xiang D.Xiao G.Y.Xiao S.Y.Xiao Y.L.Xiao Z.J.Xiao C.Xie X.H.Xie Y.Xie Y.G.Xie Y.H.Xie Z.P.Xie T.Y.Xing C.F.Xu C.J.Xu G.F.Xu H.Y.Xu M.Xu Q.J.Xu Q.N.Xu W.Xu W.L.Xu X.P.Xu Y.Xu Y.C.Xu Z.S.Xu F.Yan L.Yan W.B.Yan W.C.Yan X.Q.Yan H.J.Yang H.L.Yang H.X.Yang J.H.Yang T.Yang Y.Yang Y.F.Yang Y.F.Yang Y.X.Yang Z.W.Yang Z.P.Yao M.Ye M.H.Ye J.H.Yin Junhao Yin Z.Y.You B.X.Yu C.X.Yu G.Yu J.S.Yu M.C.Yu T.Yu X.D.Yu Y.C.Yu C.Z.Yuan J.Yuan J.Yuan L.Yuan S.C.Yuan Y.Yuan Z.Y.Yuan C.X.Yue A.A.Zafar F.R.Zeng S.H.Zeng X.Zeng Y.Zeng Y.J.Zeng Y.J.Zeng X.Y.Zhai Y.C.Zhai Y.H.Zhan A.Q.Zhang B.L.Zhang B.X.Zhang D.H.Zhang G.Y.Zhang H.Zhang H.Zhang H.C.Zhang H.H.Zhang H.H.Zhang H.Q.Zhang H.R.Zhang H.Y.Zhang J.Zhang J.Zhang J.J.Zhang J.L.Zhang J.Q.Zhang J.S.Zhang J.W.Zhang J.X.Zhang J.Y.Zhang J.Z.Zhang Jianyu Zhang L.M.Zhang Lei Zhang P.Zhang Q.Y.Zhang R.Y.Zhang S.H.Zhang Shulei Zhang X.M.Zhang X.Y Zhang X.Y.Zhang Y.Zhang Y.Zhang Y.T.Zhang Y.H.Zhang Y.M.Zhang Yan Zhang Z.D.Zhang Z.H.Zhang Z.L.Zhang Z.Y.Zhang Z.Y.Zhang Z.Z.Zhang G.Zhao J.Y.Zhao J.Z.Zhao L.Zhao L.Zhao M.G.Zhao N.Zhao R.P.Zhao S.J.Zhao Y.B.Zhao Y.X.Zhao Z.G.Zhao A.Zhemchugov B.Zheng B.M.Zheng J.P.Zheng W.J.Zheng Y.H.Zheng B.Zhong X.Zhong H.Zhou J.Y.Zhou L.P.Zhou S.Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou Y.Z.Zhou Z.C.Zhou A.N.Zhu J.Zhu K.Zhu K.J.Zhu K.S.Zhu L.Zhu L.X.Zhu S.H.Zhu T.J.Zhu W.D.Zhu Y.C.Zhu Z.A.Zhu J.H.Zou J.Zu 《Chinese Physics C》 2025年第9期1-11,共11页
By analyzing ψ(3686) data sample containing (107.7±0.6)×10^(6) events taken with the BESIII detector at the BEPCII storage ring in 2009,the χ_(c 0) resonance parameters are precisely measured using χ_(c 0... By analyzing ψ(3686) data sample containing (107.7±0.6)×10^(6) events taken with the BESIII detector at the BEPCII storage ring in 2009,the χ_(c 0) resonance parameters are precisely measured using χ_(c 0,c 2)→π^(+)π^(−)/K^(+)K^(−) events.The mass of χ_(c 0) is determined to be M (χ_(c 0))=(3415.63±0.07±0.07±0.07)MeV/c^(2),and its full width is F (χ_(c 0))=(12.52±0.12±0.13)MeV,where the first uncertainty is statistical,the second systematic,and the third for mass comes from χ_(c 2) mass uncertainty.These measurements improve the precision of χ_(c 0) mass by a factor of four and width by one order of magnitude over the previous individual measurements,and significantly boost our knowledge about the charmonium spectrum.Together with additional (345.4±2.6)×10^(6)(3686) data events taken in 2012,the decay branching fractions of χ_(c 0,c 2)→π^(+)π^(−)/K^(+)K^(−) are measured as well,with precision improved by a factor of three compared to previous measurements.These χ_(c 0) decay branching fractions provide important inputs for the study of glueballs. 展开更多
关键词 χ_(c 0) BESII CHARMONIUM resonance parameter branching fraction
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Search for radiative leptonic decay D^(+)→γe^(+)ν_(e) using deep learning
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作者 M.Ablikim M.N.Achasov +712 位作者 P.Adlarson X.C.Ai R.Aliberti A.Amoroso Q.An Y.Bai O.Bakina Y.Ban H.-R.Bao V.Batozskaya K.Begzsuren N.Berger M.Berlowski M.Bertani D.Bettoni F.Bianchi E.Bianco A.Bortone I.Boyko R.A.Briere A.Brueggemann H.Cai M.H.Cai X.Cai A.Calcaterra G.F.Cao N.Cao S.A.Cetin X.Y.Chai J.F.Chang G.R.Che Y.Z.Che G.Chelkov C.Chen C.H.Chen Chao Chen G.Chen H.S.Chen H.Y.Chen M.L.Chen S.J.Chen S.L.Chen S.M.Chen T.Chen X.R.Chen X.T.Chen X.Y.Chen Y.B.Chen Y.Q.Chen Z.J.Chen Z.K.Chen S.K.Choi X.Chu G.Cibinetto F.Cossio J.J.Cui H.L.Dai J.P.Dai A.Dbeyssi R.E.de Boer D.Dedovich C.Q.Deng Z.Y.Deng A.Denig I.Denysenko M.Destefanis F.De Mori B.Ding X.X.Ding Y.Ding Y.Ding Y.X.Ding J.Dong L.Y.Dong M.Y.Dong X.Dong M.C.Du S.X.Du S.X.Du Y.Y.Duan Z.H.Duan P.Egorov G.F.Fan J.J.Fan Y.H.Fan J.Fang J.Fang S.S.Fang W.X.Fang Y.Q.Fang R.Farinelli L.Fava F.Feldbauer G.Felici C.Q.Feng Y.T.Feng M.Fritsch C.D.Fu J.L.Fu Y.W.Fu H.Gao X.B.Gao Y.Gao Y.N.Gao Y.N.Gao Y.Y.Gao S.Garbolino I.Garzia P.T.Ge Z.W.Ge C.Geng E.M.Gersabeck A.Gilman K.Goetzen J.D.Gong L.Gong W.X.Gong W.Gradl S.Gramigna M.Greco M.H.Gu Y.T.Gu C.Y.Guan A.Q.Guo L.B.Guo M.J.Guo R.P.Guo Y.P.Guo A.Guskov J.Gutierrez K.L.Han T.T.Han F.Hanisch K.D.Hao X.Q.Hao F.A.Harris K.K.He K.L.He F.H.Heinsius C.H.Heinz Y.K.Heng C.Herold T.Holtmann P.C.Hong G.Y.Hou X.T.Hou Y.R.Hou Z.L.Hou H.M.Hu J.F.Hu Q.P.Hu S.L.Hu T.Hu Y.Hu Z.M.Hu G.S.Huang K.X.Huang L.Q.Huang P.Huang X.T.Huang Y.P.Huang Y.S.Huang T.Hussain N.Hüsken N.in der Wiesche J.Jackson Q.Ji Q.P.Ji W.Ji X.B.Ji X.L.Ji Y.Y.Ji Z.K.Jia D.Jiang H.B.Jiang P.C.Jiang S.J.Jiang T.J.Jiang X.S.Jiang Y.Jiang J.B.Jiao J.K.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing X.M.Jing T.Johansson S.Kabana N.Kalantar-Nayestanaki X.L.Kang X.S.Kang M.Kavatsyuk B.C.Ke V.Khachatryan A.Khoukaz R.Kiuchi O.B.Kolcu B.Kopf M.Kuessner X.Kui N.Kumar A.Kupsc W.Kühn Q.Lan W.N.Lan T.T.Lei M.Lellmann T.Lenz C.Li C.Li C.Li C.H.Li C.K.Li D.M.Li F.Li G.Li H.B.Li H.J.Li H.N.Li Hui Li J.R.Li J.S.Li K.Li K.L.Li K.L.Li L.J.Li Lei Li M.H.Li M.R.Li P.L.Li P.R.Li Q.M.Li Q.X.Li R.Li S.X.Li T.Li T.Y.Li W.D.Li W.G.Li X.Li X.H.Li X.L.Li X.Y.Li X.Z.Li Y.Li Y.G.Li Y.P.Li Z.J.Li Z.Y.Li C.Liang H.Liang Y.F.Liang Y.T.Liang G.R.Liao L.B.Liao M.H.Liao Y.P.Liao J.Libby A.Limphirat C.C.Lin C.X.Lin D.X.Lin L.Q.Lin T.Lin B.J.Liu B.X.Liu c.liu C.X.Liu F.Liu F.H.Liu Feng Liu G.M.Liu H.Liu H.B.Liu H.H.Liu H.M.Liu Huihui Liu J.B.Liu J.J.Liu K.Liu K.Liu K.Y.Liu Ke Liu L.Liu L.c.liu Lu Liu M.H.Liu P.L.Liu Q.Liu S.B.Liu T.Liu W.K.Liu W.M.Liu W.T.Liu X.Liu X.Liu X.L.Liu X.Y.Liu Y.Liu Y.Liu Y.Liu Y.B.Liu Z.A.Liu Z.D.Liu Z.Q.Liu X.C.Lou F.X.Lu H.J.Lu J.G.Lu Y.Lu Y.H.Lu Y.P.Lu Z.H.Lu C.L.Luo J.R.Luo J.S.Luo M.X.Luo T.Luo X.L.Luo Z.Y.Lv X.R.Lyu Y.F.Lyu Y.H.Lyu F.C.Ma H.Ma H.L.Ma J.L.Ma L.L.Ma L.R.Ma Q.M.Ma R.Q.Ma R.Y.Ma T.Ma X.T.Ma X.Y.Ma Y.M.Ma F.E.Maas I.MacKay M.Maggiora S.Malde Q.A.Malik Y.J.Mao Z.P.Mao S.Marcello F.M.Melendi Y.H.Meng Z.X.Meng J.G.Messchendorp G.Mezzadri H.Miao T.J.Min R.E.Mitchell X.H.Mo B.Moses N.Yu.Muchnoi J.Muskalla Y.Nefedov F.Nerling L.S.Nie I.B.Nikolaev Z.Ning S.Nisar Q.L.Niu W.D.Niu S.L.Olsen Q.Ouyang S.Pacetti X.Pan Y.Pan A.Pathak Y.P.Pei M.Pelizaeus H.P.Peng Y.Y.Peng K.Peters J.L.Ping R.G.Ping S.Plura F.Z.Qi H.R.Qi M.Qi S.Qian W.B.Qian C.F.Qiao J.H.Qiao J.J.Qin J.L.Qin L.Q.Qin L.Y.Qin P.B.Qin X.P.Qin X.S.Qin Z.H.Qin J.F.Qiu Z.H.Qu C.F.Redmer A.Rivetti M.Rolo G.Rong S.S.Rong F.Rosini Ch.Rosner M.Q.Ruan S.N.Ruan N.Salone A.Sarantsev Y.Schelhaas K.Schoenning M.Scodeggio K.Y.Shan W.Shan X.Y.Shan Z.J.Shang J.F.Shangguan L.G.Shao M.Shao C.P.Shen H.F.Shen W.H.Shen X.Y.Shen B.A.Shi H.Shi J.L.Shi J.Y.Shi S.Y.Shi X.Shi H.L.Song J.J.Song T.Z.Song W.M.Song Y.J.Song Y.X.Song S.Sosio S.Spataro F.Stieler S.S Su Y.J.Su G.B.Sun G.X.Sun H.Sun H.K.Sun J.F.Sun K.Sun L.Sun S.S.Sun T.Sun Y.C.Sun Y.H.Sun Y.J.Sun Y.Z.Sun Z.Q.Sun Z.T.Sun C.J.Tang G.Y.Tang J.Tang J.J.Tang L.F.Tang Y.A.Tang L.Y.Tao M.Tat J.X.Teng J.Y.Tian W.H.Tian Y.Tian Z.F.Tian I.Uman B.Wang B.Wang Bo Wang C.Wang Cong Wang D.Y.Wang H.J.Wang J.J.Wang K.Wang L.L.Wang L.W.Wang M.Wang M.Wang N.Y.Wang S.Wang T.Wang T.J.Wang W.Wang W.Wang W.P.Wang X.Wang X.F.Wang X.J.Wang X.L.Wang X.N.Wang Y.Wang Y.D.Wang Y.F.Wang Y.H.Wang Y.J.Wang Y.L.Wang Y.N.Wang Y.Q.Wang Yaqian Wang Yi Wang Yuan Wang Z.Wang Z.L.Wang Z.L.Wang Z.Q.Wang Z.Y.Wang D.H.Wei H.R.Wei F.Weidner S.P.Wen Y.R.Wen U.Wiedner G.Wilkinson M.Wolke C.Wu J.F.Wu L.H.Wu L.J.Wu L.J.Wu Lianjie Wu S.G.Wu S.M.Wu X.Wu X.H.Wu Y.J.Wu Z.Wu L.Xia X.M.Xian B.H.Xiang D.Xiao G.Y.Xiao H.Xiao Y.L.Xiao Z.J.Xiao C.Xie K.J.Xie X.H.Xie Y.Xie Y.G.Xie Y.H.Xie Z.P.Xie T.Y.Xing C.F.Xu C.J.Xu G.F.Xu H.Y.Xu H.Y.Xu M.Xu Q.J.Xu Q.N.Xu T.D.Xu W.Xu W.L.Xu X.P.Xu Y.Xu Y.Xu Y.C.Xu Z.S.Xu F.Yan H.Y.Yan L.Yan W.B.Yan W.C.Yan W.H.Yan W.P.Yan X.Q.Yan H.J.Yang H.L.Yang H.X.Yang J.H.Yang R.J.Yang T.Yang Y.Yang Y.F.Yang Y.H.Yang Y.Q.Yang Y.X.Yang Y.Z.Yang M.Ye M.H.Ye Z.J.Ye Junhao Yin Z.Y.You B.X.Yu C.X.Yu G.Yu J.S.Yu L.Q.Yu M.C.Yu T.Yu X.D.Yu Y.C.Yu C.Z.Yuan H.Yuan J.Yuan J.Yuan L.Yuan S.C.Yuan X.Q.Yuan Y.Yuan Z.Y.Yuan C.X.Yue Ying Yue A.A.Zafar S.H.Zeng X.Zeng Y.Zeng Y.J.Zeng Y.J.Zeng X.Y.Zhai Y.H.Zhan A.Q.Zhang B.L.Zhang B.X.Zhang D.H.Zhang G.Y.Zhang G.Y.Zhang H.Zhang H.Zhang H.C.Zhang H.H.Zhang H.Q.Zhang H.R.Zhang H.Y.Zhang J.Zhang J.Zhang J.J.Zhang J.L.Zhang J.Q.Zhang J.S.Zhang J.W.Zhang J.X.Zhang J.Y.Zhang J.Z.Zhang Jianyu Zhang L.M.Zhang Lei Zhang N.Zhang P.Zhang Q.Zhang Q.Y.Zhang R.Y.Zhang S.H.Zhang Shulei Zhang X.M.Zhang X.Y Zhang X.Y.Zhang Y.Zhang Y.Zhang Y.T.Zhang Y.H.Zhang Y.M.Zhang Y.P.Zhang Z.D.Zhang Z.H.Zhang Z.L.Zhang Z.L.Zhang Z.X.Zhang Z.Y.Zhang Z.Y.Zhang Z.Z.Zhang Zh.Zh.Zhang G.Zhao J.Y.Zhao J.Z.Zhao L.Zhao L.Zhao M.G.Zhao N.Zhao R.P.Zhao S.J.Zhao Y.B.Zhao Y.L.Zhao Y.X.Zhao Z.G.Zhao A.Zhemchugov B.Zheng B.M.Zheng J.P.Zheng W.J.Zheng X.R.Zheng Y.H.Zheng B.Zhong C.Zhong H.Zhou J.Q.Zhou J.Y.Zhou S.Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou Y.Z.Zhou A.N.Zhu J.Zhu K.Zhu K.J.Zhu K.S.Zhu L.Zhu L.X.Zhu S.H.Zhu T.J.Zhu W.D.Zhu W.D.Zhu W.J.Zhu W.Z.Zhu Y.C.Zhu Z.A.Zhu X.Y.Zhuang J.H.Zou J.Zu 《Chinese Physics C》 2025年第8期1-15,共15页
Using 20.3 fb^(-1)of e^(+)e^(-)annihilation data collected at a center-of-mass energy of 3.773 GeV with the BESⅢdetector,we report on an improved search for the radiative leptonic decay D^(+)→γe^(+)ve.An upper limi... Using 20.3 fb^(-1)of e^(+)e^(-)annihilation data collected at a center-of-mass energy of 3.773 GeV with the BESⅢdetector,we report on an improved search for the radiative leptonic decay D^(+)→γe^(+)ve.An upper limit on its partial branching fraction for photon energies E_(γ)>10 MeV was determined to be 1.2×10^(-5)at a 90%confidence level;this excludes most current theoretical predictions.A sophisticated deep learning approach,which includes thorough validation and is based on the Transformer architecture,was implemented to efficiently distinguish the signal from massive backgrounds. 展开更多
关键词 charmed hadron radiative leptonic decay BESIl experiment deep learning
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Precise measurements of the cosmic ray proton energy spectrum in the“knee”region
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作者 Zhen Cao F.Aharonian +312 位作者 Y.X.Bai Y.W.Bao D.Bastieri X.J.Bi Y.J.Bi W.Bian A.V.Bukevich C.M.Cai W.Y.Cao Zhe Cao J.Chang J.F.Chang A.M.Chen E.S.Chen G.H.Chen H.X.Chen Liang Chen Long Chen M.J.Chen M.L.Chen Q.H.Chen S.Chen S.H.Chen S.Z.Chen T.L.Chen X.B.Chen X.J.Chen Y.Chen N.Cheng Y.D.Cheng M.C.Chu M.Y.Cui S.W.Cui X.H.Cui Y.D.Cui B.Z.Dai H.L.Dai Z.G.Dai Y.X.Diao X.Q.Dong K.K.Duan J.H.Fan Y.Z.Fan J.Fang J.H.Fang K.Fang C.F.Feng H.Feng L.Feng S.H.Feng X.T.Feng Y.Feng Y.L.Feng S.Gabici B.Gao C.D.Gao Q.Gao W.Gao W.K.Gao M.M.Ge T.T.Ge L.S.Geng G.Giacinti G.H.Gong Q.B.Gou M.H.Gu F.L.Guo J.Guo X.L.Guo Y.Q.Guo Y.Y.Guo Y.A.Han O.A.Hannuksela M.Hasan H.H.He H.N.He J.Y.He X.Y.He Y.He S.Hernández-Cadena B.W.Hou C.Hou X.Hou H.B.Hu S.C.Hu C.Huang D.H.Huang J.J.Huang T.Q.Huang W.J.Huang X.T.Huang X.Y.Huang Y.Huang Y.Y.Huang X.L.Ji H.Y.Jia K.Jia H.B.Jiang K.Jiang X.W.Jiang Z.J.Jiang M.Jin S.Kaci M.M.Kang I.Karpikov D.Khangulyan D.Kuleshov K.Kurinov B.B.Li Cheng Li Cong Li D.Li F.Li H.B.Li H.C.Li Jian Li Jie Li K.Li L.Li R.L.Li S.D.Li T.Y.Li W.L.Li X.R.Li Xin Li Y.Li Y.Z.Li Zhe Li Zhuo Li E.W.Liang Y.F.Liang S.J.Lin P.Lipari B.Liu c.liu D.Liu D.B.Liu H.Liu H.D.Liu J.Liu J.L.Liu J.R.Liu M.Y.Liu R.Y.Liu S.M.Liu W.Liu X.Liu Y.Liu Y.Liu Y.N.Liu Y.Q.Lou Q.Luo Y.Luo H.K.Lv B.Q.Ma L.L.Ma X.H.Ma J.R.Mao Z.Min W.Mitthumsiri G.B.Mou H.J.Mu A.Neronov K.C.Y.Ng M.Y.Ni L.Nie L.J.Ou P.Pattarakijwanich Z.Y.Pei J.C.Qi M.Y.Qi J.J.Qin A.Raza C.Y.Ren D.Ruffolo A.Sáiz D.Semikoz L.Shao O.Shchegolev Y.Z.Shen X.D.Sheng Z.D.Shi F.W.Shu H.C.Song V.Stepanov Y.Su D.X.Sun H.Sun Q.N.Sun X.N.Sun Z.B.Sun N.H.Tabasam J.Takata P.H.T.Tam H.B.Tan Q.W.Tang R.Tang Z.B.Tang W.W.Tian C.N.Tong L.H.Wan C.Wang G.W.Wang H.G.Wang J.C.Wang K.Wang Kai Wang Kai Wang L.P.Wang L.Y.Wang L.Y.Wang R.Wang W.Wang X.G.Wang X.J.Wang X.Y.Wang Y.Wang Y.D.Wang Z.H.Wang Z.X.Wang Zheng Wang D.M.Wei J.J.Wei Y.J.Wei T.Wen S.S.Weng C.Y.Wu H.R.Wu Q.W.Wu S.Wu X.F.Wu Y.S.Wu S.Q.Xi J.Xia J.J.Xia G.M.Xiang D.X.Xiao G.Xiao Y.L.Xin Y.Xing D.R.Xiong Z.Xiong D.L.Xu R.F.Xu R.X.Xu W.L.Xu L.Xue D.H.Yan T.Yan C.W.Yang C.Y.Yang F.F.Yang L.L.Yang M.J.Yang R.Z.Yang W.X.Yang Z.H.Yang Z.G.Yao X.A.Ye L.Q.Yin N.Yin X.H.You Z.Y.You Q.Yuan H.Yue H.D.Zeng T.X.Zeng W.Zeng X.T.Zeng M.Zha B.B.Zhang B.T.Zhang C.Zhang F.Zhang H.Zhang H.M.Zhang H.Y.Zhang J.L.Zhang Li Zhang P.F.Zhang P.P.Zhang R.Zhang S.R.Zhang S.S.Zhang W.Y.Zhang X.Zhang X.P.Zhang Yi Zhang Yong Zhang Z.P.Zhang J.Zhao L.Zhao L.Z.Zhao S.P.Zhao X.H.Zhao Z.H.Zhao F.Zheng W.J.Zhong B.Zhou H.Zhou J.N.Zhou M.Zhou P.Zhou R.Zhou X.X.Zhou X.X.Zhou B.Y.Zhu C.G.Zhu F.R.Zhu H.Zhu K.J.Zhu Y.C.Zou X.Zuo 《Science Bulletin》 2025年第24期4173-4180,共8页
We report the high-purity identification of cosmic-ray(CR)protons and a precise measurement of their energy spectrum from 0.15 to 12 PeV using the Large High Altitude Air Shower Observatory(LHAASO).Abundant event stat... We report the high-purity identification of cosmic-ray(CR)protons and a precise measurement of their energy spectrum from 0.15 to 12 PeV using the Large High Altitude Air Shower Observatory(LHAASO).Abundant event statistics,combined with the simultaneous detection of electrons/photons,muons,and Cherenkov light in air showers,enable spectroscopic measurements with statistical and systematic precision comparable to satellite data at lower energies.The proton spectrum shows significant hardening relative to low-energy extrapolations,culminating at 3 PeV,followed by sharp softening.This distinct spectral structure closely aligned with the knee in the all-particle spectrum points to the emergence of a new CR component at PeV energies that might be linked to the dozens of PeVatrons recently discovered by LHAASO,and offers crucial clues to the origin of Galactic cosmic rays. 展开更多
关键词 Proton spectrum Cosmic rays Large High Altitude Air Shower Observatory Cosmic ray knee
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Search for the lepton number violation decay ϕ→π^(+)π^(+)e^(−)e^(−)via J/ψ→ϕη^(*)
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作者 M.Ablikim M.N.Achasov +627 位作者 P.Adlarson O.Afedulidis X.C.Ai R.Aliberti A.Amoroso M.R.An Q.An Y.Bai O.Bakina I.Balossino Y.Ban H.-R.Bao V.Batozskaya K.Begzsuren N.Berger M.Berlowski M.Bertani D.Bettoni F.Bianchi E.Bianco A.Bortone I.Boyko R.A.Briere A.Brueggemann H.Cai X.Cai A.Calcaterra G.F.Cao N.Cao S.A.Cetin J.F.Chang G.R.Che Y.Z.Che G.Chelkov C.Chen Chao Chen G.Chen H.S.Chen M.L.Chen S.J.Chen S.L.Chen S.M.Chen T.Chen X.R.Chen X.T.Chen Y.B.Chen Y.Q.Chen Z.J.Chen Z.Y.Chen S.K.Choi G.Cibinetto S.C.Coen F.Cossio J.J.Cui H.L.Dai J.P.Dai A.Dbeyssi R.E.de Boer D.Dedovich Z.Y.Deng A.Denig I.Denysenko M.Destefanis F.De Mori B.Ding X.X.Ding Y.Ding Y.Ding J.Dong L.Y.Dong M.Y.Dong X.Dong M.C.Du S.X.Du Z.H.Duan P.Egorov Y.H.Fan J.Fang S.S.Fang W.X.Fang Y.Fang Y.Q.Fang R.Farinelli L.Fava F.Feldbauer G.Felici C.Q.Feng J.H.Feng K.Fischer M.Fritsch C.D.Fu J.L.Fu Y.W.Fu H.Gao Y.N.Gao Yang Gao S.Garbolino I.Garzia L.Ge P.T.Ge Z.W.Ge C.Geng E.M.Gersabeck A.Gilman K.Goetzen L.Gong W.X.Gong W.Gradl S.Gramigna M.Greco M.H.Gu Y.T.Gu C.Y.Guan A.Q.Guo L.B.Guo M.J.Guo R.P.Guo Y.P.Guo A.Guskov J.Gutierrez T.T.Han W.Y.Han X.Q.Hao F.A.Harris K.K.He K.L.He F.H.Heinsius C.H.Heinz Y.K.Heng C.Herold T.Holtmann P.C.Hong G.Y.Hou X.T.Hou Y.R.Hou Z.L.Hou B.Y.Hu H.M.Hu J.F.Hu T.Hu Y.Hu G.S.Huang K.X.Huang L.Q.Huang X.T.Huang Y.P.Huang T.Hussain F.Hölzken N.Hüsken N.in der Wiesche J.Jackson S.Jaeger S.Janchiv Q.Ji Q.P.Ji X.B.Ji X.L.Ji Y.Y.Ji X.Q.Jia Z.K.Jia H.B.Jiang P.C.Jiang S.S.Jiang T.J.Jiang X.S.Jiang Y.Jiang J.B.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing X.M.Jing T.Johansson S.Kabana N.Kalantar-Nayestanaki X.L.Kang X.S.Kang M.Kavatsyuk B.C.Ke V.Khachatryan A.Khoukaz R.Kiuchi R.Kliemt O.B.Kolcu B.Kopf M.Kuessner X.Kui N.Kumar A.Kupsc W.Kühn J.J.Lane P.Larin A.Lavania L.Lavezzi T.T.Lei Z.H.Lei M.Lellmann T.Lenz C.Li C.Li C.H.Li Cheng Li D.M.Li F.Li G.Li H.B.Li H.J.Li H.N.Li Hui Li J.R.Li J.S.Li J.W.Li K.Li K.L.Li L.J.Li L.K.Li Lei Li M.H.Li P.R.Li Q.X.Li S.X.Li T.Li W.D.Li W.G.Li X.H.Li X.L.Li X.Y.Li Y.G.Li Z.J.Li Z.X.Li C.Liang H.Liang H.Liang Y.F.Liang Y.T.Liang G.R.Liao L.Z.Liao Y.P.Liao J.Libby A.Limphirat D.X.Lin T.Lin B.J.Liu B.X.Liu c.liu C.X.Liu F.Liu F.H.Liu Feng Liu G.M.Liu H.Liu H.B.Liu H.H.Liu H.M.Liu Huihui Liu J.B.Liu J.Y.Liu K.Liu K.Y.Liu Ke Liu L.Liu L.c.liu Lu Liu M.H.Liu P.L.Liu Q.Liu S.B.Liu T.Liu W.K.Liu W.M.Liu X.Liu Y.Liu Y.Liu Y.B.Liu Z.A.Liu Z.Q.Liu X.C.Lou F.X.Lu H.J.Lu J.G.Lu X.L.Lu Y.Lu Y.P.Lu Z.H.Lu C.L.Luo M.X.Luo T.Luo X.L.Luo X.R.Lyu Y.F.Lyu F.C.Ma H.Ma H.L.Ma J.L.Ma L.L.Ma M.M.Ma Q.M.Ma R.Q.Ma X.Y.Ma Y.M.Ma F.E.Maas M.Maggiora S.Malde A.Mangoni Y.J.Mao Z.P.Mao S.Marcello Z.X.Meng J.G.Messchendorp G.Mezzadri H.Miao T.J.Min R.E.Mitchell X.H.Mo B.Moses N.Yu.Muchnoi J.Muskalla Y.Nefedov F.Nerling I.B.Nikolaev Z.Ning S.Nisar Q.L.Niu W.D.Niu Y.Niu S.L.Olsen Q.Ouyang S.Pacetti X.Pan Y.Pan P.Patteri Y.P.Pei M.Pelizaeus H.P.Peng Y.Y.Peng K.Peters J.L.Ping R.G.Ping S.Plura V.Prasad F.Z.Qi H.Qi H.R.Qi M.Qi T.Y.Qi S.Qian W.B.Qian C.F.Qiao X.K.Qiao J.J.Qin L.Q.Qin L.Y.Qin X.P.Qin X.S.Qin Z.H.Qin J.F.Qiu S.Q.Qu F.Redmer K.J.Ren A.Rivetti M.Rolo G.Rong Ch.Rosner M.Q.Ruan S.N.Ruan N.Salone A.Sarantsev Y.Schelhaas K.Schoenning M.Scodeggio K.Y.Shan W.Shan X.Y.Shan J.F.Shangguan L.G.Shao M.Shao C.P.Shen H.F.Shen W.H.Shen X.Y.Shen B.A.Shi H.Shi H.C.Shi J.L.Shi J.Y.Shi Q.Q.Shi X.Shi J.J.Song T.Z.Song W.M.Song Y.J.Song Y.X.Song S.Sosio S.Spataro F.Stieler Y.J.Su G.B.Sun G.X.Sun H.Sun H.K.Sun J.F.Sun K.Sun L.Sun S.S.Sun T.Sun W.Y.Sun Y.Sun Y.J.Sun Y.Z.Sun Z.T.Sun C.J.Tang G.Y.Tang J.Tang Y.A.Tang L.Y.Tao Q.T.Tao M.Tat J.X.Teng V.Thoren W.H.Tian W.H.Tian Y.Tian Z.F.Tian I.Uman Y.Wan S.J.Wang B.Wang B.L.Wang Bo Wang C.W.Wang D.Y.Wang F.Wang H.J.Wang J.P.Wang K.Wang L.L.Wang L.W.Wang M.Wang N.Y.Wang S.Wang S.Wang T.Wang T.J.Wang W.Wang W.Wang W.P.Wang X.Wang X.F.Wang X.J.Wang X.L.Wang Y.Wang Y.D.Wang Y.F.Wang Y.L.Wang Y.N.Wang Y.Q.Wang Yaqian Wang Yi Wang Z.Wang Z.L.Wang Z.Y.Wang Ziyi Wang D.H.Wei F.Weidner S.P.Wen Wenzel U.Wiedner G.Wilkinson M.Wolke L.Wollenberg C.Wu J.F.Wu L.H.Wu L.J.Wu X.Wu X.H.Wu Y.Wu Y.H.Wu Y.J.Wu Z.Wu L.Xia X.M.Xian T.Xiang D.Xiao G.Y.Xiao S.Y.Xiao Y.L.Xiao Z.J.Xiao C.Xie X.H.Xie Y.Xie Y.G.Xie Y.H.Xie Z.P.Xie T.Y.Xing C.F.Xu C.J.Xu G.F.Xu H.Y.Xu M.Xu Q.J.Xu Q.N.Xu W.Xu W.L.Xu X.P.Xu Y.Xu Y.C.Xu Z.P.Xu Z.S.Xu F.Yan L.Yan W.B.Yan W.C.Yan X.Q.Yan H.J.Yang H.L.Yang H.X.Yang T.Yang Y.Yang Y.F.Yang Y.F.Yang Y.X.Yang Z.W.Yang Z.P.Yao M.Ye M.H.Ye J.H.Yin Z.Y.You B.X.Yu C.X.Yu G.Yu J.S.Yu T.Yu X.D.Yu Y.C.Yu C.Z.Yuan L.Yuan S.C.Yuan Y.Yuan Z.Y.Yuan C.X.Yue A.A.Zafar F.R.Zeng S.H.Zeng X.Zeng Y.Zeng X.Y.Zhai Y.C.Zhai Y.H.Zhan A.Q.Zhang B.L.Zhang B.X.Zhang D.H.Zhang G.Y.Zhang H.Zhang H.C.Zhang H.H.Zhang H.H.Zhang H.Q.Zhang H.Y.Zhang J.Zhang J.Zhang J.J.Zhang J.L.Zhang J.Q.Zhang J.W.Zhang J.X.Zhang J.Y.Zhang J.Z.Zhang Jianyu Zhang L.M.Zhang Lei Zhang P.Zhang Q.Y.Zhang S.H.Zhang Shulei Zhang X.D.Zhang X.M.Zhang X.Y.Zhang Y.Zhang Y.Zhang Y.T.Zhang Y.H.Zhang Y.X.Zhang Yan Zhang Z.D.Zhang Z.H.Zhang Z.L.Zhang Z.Y.Zhang Z.Y.Zhang G.Zhao J.Y.Zhao J.Z.Zhao L.Zhao Lei Zhao M.G.Zhao R.P.Zhao S.J.Zhao Y.B.Zhao Y.X.Zhao Z.G.Zhao A.Zhemchugov B.Zheng J.P.Zheng W.J.Zheng Y.H.Zheng B.Zhong X.Zhong L.P.Zhou S.Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou Y.Z.Zhou J.Zhu K.Zhu K.J.Zhu L.Zhu L.X.Zhu S.H.Zhu S.Q.Zhu T.J.Zhu Y.C.Zhu Z.A.Zhu J.H.Zou J.Zu BESIII Collaboration 《Chinese Physics C》 2025年第4期1-10,共10页
Using an electron-positron collision data sample corresponding to(1.0087±0.0044)×10^(10)events collected using the BESIII detector at the BEPCII collider,we firstly search for the lepton number violation de... Using an electron-positron collision data sample corresponding to(1.0087±0.0044)×10^(10)events collected using the BESIII detector at the BEPCII collider,we firstly search for the lepton number violation decayφ→π^(+)π^(+)e^(-)e^(-)via J/ψ→φη.No obviously signals are found.The upper limit on the branching fraction ofφ→π^(+)π^(+)e^(-)e^(-)is set to be 1.3×10^(-5)at the 90%confidence level. 展开更多
关键词 Lepton number violation matter anti-matter asymmetry neutrinoless double beta decay
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Deep view of composite SNR CTA1 with LHAASO inγ-rays up to 300 TeV
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作者 Zhen Cao F.A.haronian +297 位作者 Axikegu Y.X.Bai Y.W.Bao D.Bastieri X.J.Bi Y.J.Bi W.Bian A.V.Bukevich Q.Cao W.Y.Cao Zhe Cao J.Chang J.F.Chang A.M.Chen E.S.Chen H.X.Chen Liang Chen Lin Chen Long Chen M.J.Chen M.L.Chen Q.H.Chen S.Chen S.H.Chen S.Z.Chen T.L.Chen Y.Chen N.Cheng Y.D.Cheng M.C.Chu M.Y.Cui S.W.Cui X.H.Cui Y.D.Cui B.Z.Dai H.L.Dai Z.G.Dai Danzengluobu X.Q.Dong K.K.Duan J.H.Fan Y.Z.Fan J.Fang J.H.Fang K.Fang C.F.Feng H.Feng L.Feng S.H.Feng X.T.Feng Y.Feng Y.L.Feng S.Gabici B.Gao C.D.Gao Q.Gao W.Gao W.K.Gao M.M.Ge T.T.Ge L.S.Geng G.Giacinti G.H.Gong Q.B.Gou M.H.Gu F.L.Guo J.Guo X.L.Guo Y.Q.Guo Y.Y.Guo Y.A.Han O.A.Hannuksela M.Hasan H.H.He H.N.He J.Y.He Y.He Y.K.Hor B.W.Hou C.Hou X.Hou H.B.Hu Q.Hu S.C.Hu C.Huang D.H.Huang T.Q.Huang W.J.Huang X.T.Huang X.Y.Huang Y.Huang Y.Y.Huang X.L.Ji H.Y.Jia K.Jia H.B.Jiang K.Jiang X.W.Jiang Z.J.Jiang M.Jin M.M.Kang I.Karpikov D.K.hangulyan D.Kuleshov K.Kurinov B.B.Li C.M.Li Cheng Li Cong Li D.Li F.Li H.B.Li H.C.Li Jian Li Jie Li K.Li S.D.Li W.L.Li W.L.Li X.R.Li Xin Li Y.Z.Li Zhe Li Zhuo Li E.W.Liang Y.F.Liang S.J.Lin B.Liu c.liu D.Liu D.B.Liu H.Liu H.D.Liu J.Liu J.L.Liu M.Y.Liu R.Y.Liu S.M.Liu W.Liu Y.Liu Y.N.Liu Q.Luo Y.Luo H.K.Lv B.Q.Ma L.L.Ma X.H.Ma J.R.Mao Z.Min W.Mitthumsiri H.J.Mu Y.C.Nan A.Neronov K.C.Y.Ng L.J.Ou P.Pattarakijwanich Z.Y.Pei J.C.Qi M.Y.Qi B.Q.Qiao J.J.Qin A.Raza D.Ruffolo A.Saiz´ M.Saeed D.Semikoz L.Shao O.Shchegolev X.D.Sheng F.W.Shu H.C.Song Yu V.Stenkin V.Stepanov Y.Su D.X.Sun Q.N.Sun X.N.Sun Z.B.Sun J.Takata P.H.T.Tam Q.W.Tang R.Tang Z.B.Tang W.W.Tian L.H.Wan C.Wang C.B.Wang G.W.Wang H.G.Wang H.H.Wang J.C.Wang Kai Wang Kai Wang L.P.Wang L.Y.Wang P.H.Wang R.Wang W.Wang X.G.Wang X.Y.Wang Y.Wang Y.D.Wang Y.J.Wang Z.H.Wang Z.X.Wang Zhen Wang Zheng Wang D.M.Wei J.J.Wei Y.J.Wei T.Wen C.Y.Wu H.R.Wu Q.W.Wu S.Wu X.F.Wu Y.S.Wu S.Q.Xi J.Xia G.M.Xiang D.X.Xiao G.Xiao Y.L.Xin Y.Xing D.R.Xiong Z.Xiong D.L.Xu R.F.Xu R.X.Xu W.L.Xu L.Xue D.H.Yan J.Z.Yan T.Yan C.W.Yang C.Y.Yang F.Yang F.F.Yang L.L.Yang M.J.Yang R.Z.Yang W.X.Yang Y.H.Yao Z.G.Yao L.Q.Yin N.Yin X.H.You Z.Y.You Y.H.Yu Q.Yuan H.Yue H.D.Zeng T.X.Zeng W.Zeng M.Zha B.B.Zhang F.Zhang H.Zhang H.M.Zhang H.Y.Zhang J.L.Zhang Li Zhang P.F.Zhang P.P.Zhang R.Zhang S.B.Zhang S.R.Zhang S.S.Zhang X.Zhang X.P.Zhang Y.F.Zhang Yi Zhang Yong Zhang B.Zhao J.Zhao L.Zhao L.Z.Zhao S.P.Zhao X.H.Zhao F.Zheng W.J.Zhong B.Zhou H.Zhou J.N.Zhou M.Zhou P.Zhou R.Zhou X.X.Zhou X.X.Zhou B.Y.Zhu C.G.Zhu F.R.Zhu H.Zhu K.J.Zhu Y.C.Zou X.Zuo B.Li The LHAASO Collaboration 《Science China(Physics,Mechanics & Astronomy)》 2025年第7期13-26,共14页
The ultra-high-energy(UHE)gamma-ray source 1LHAASO J0007+7303u is positionally associated with the composite SNR CTA1 that is located at high Galactic Latitude b≈10.5°.This provides a rare opportunity to spatial... The ultra-high-energy(UHE)gamma-ray source 1LHAASO J0007+7303u is positionally associated with the composite SNR CTA1 that is located at high Galactic Latitude b≈10.5°.This provides a rare opportunity to spatially resolve the component of the pulsar wind nebula(PWN)and supernova remnant(SNR)at UHE.This paper conducted a dedicated data analysis of 1LHAASO J0007+7303u using the data collected from December 2019 to July 2023.This source is well detected with significances of 21σand 17σat 8-100 TeV and>100 TeV,respectively.The corresponding extensions are determined to be 0.23°±0.03°and 0.17°±0.03°.The emission is proposed to originate from the relativistic electrons accelerated within the PWN of PSR J0007+7303.The energy spectrum is well described by a power-law with an exponential cutoff function dN/dE=(42.4±4.1)(E/20TeV)^(-2.31+0.11)exp(-E/(110±25Tev))TeV-1 cm^(-2)s^(-1)in the energy range from 8 to 300 TeV,implying a steady-state parent electron spectrum dN_(e)/dE_(e)∝(E_(e)/100TeV)^(-3.13±0.16)exp[(-E_(e)/(373±70TeV))^(2)]at energies above≈50 TeV.The cutoff energy of the electron spectrum is roughly equal to the expected current maximum energy of particles accelerated at the PWN terminal shock.Combining the X-ray and gamma-ray emission,the current space-averaged magnetic field can be limited to≈4.5μG.To satisfy the multi-wavelength spectrum and the y-ray extensions,the transport of relativistic particles within the PWN is likely dominated by the advection process under the free-expansion phase assumption. 展开更多
关键词 PWN Γ-RAY UHE
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Search for η_(1)(1855)in χ_(cJ)→ηηη′decays
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作者 M.Ablikim M.N.Achasov +714 位作者 P.Adlarson X.C.Ai R.Aliberti A.Amoroso Q.An Y.Bai O.Bakina Y.Ban H.-R.Bao V.Batozskaya K.Begzsuren N.Berger M.Berlowski M.Bertani D.Bettoni F.Bianchi E.Bianco A.Bortone I.Boyko R.A.Briere A.Brueggemann H.Cai M.H.Cai X.Cai A.Calcaterra G.F.Cao N.Cao S.A.Cetin X.Y.Chai J.F.Chang G.R.Che Y.Z.Che C.H.Chen Chao Chen G.Chen H.S.Chen H.Y.Chen M.L.Chen S.J.Chen S.L.Chen S.M.Chen T.Chen X.R.Chen X.T.Chen X.Y.Chen Y.B.Chen Y.Q.Chen Y.Q.Chen Z.Chen Z.J.Chen Z.K.Chen S.K.Choi X.Chu G.Cibinetto F.Cossio J.Cottee-Meldrum J.J.Cui H.L.Dai J.P.Dai A.Dbeyssi R.E.de Boer D.Dedovich C.Q.Deng Z.Y.Deng A.Denig I.Denysenko M.Destefanis F.De Mori B.Ding X.X.Ding Y.Ding Y.Ding Y.X.Ding J.Dong L.Y.Dong M.Y.Dong X.Dong M.C.Du S.X.Du S.X.Du Y.Y.Duan P.Egorov G.F.Fan J.J.Fan Y.H.Fan J.Fang J.Fang S.S.Fang W.X.Fang Y.Q.Fang R.Farinelli L.Fava F.Feldbauer G.Felici C.Q.Feng J.H.Feng L.Feng Q.X.Feng Y.T.Feng M.Fritsch C.D.Fu J.L.Fu Y.W.Fu H.Gao X.B.Gao Y.Gao Y.N.Gao Y.N.Gao Y.Y.Gao S.Garbolino I.Garzia P.T.Ge Z.W.Ge C.Geng E.M.Gersabeck A.Gilman K.Goetzen J.D.Gong L.Gong W.X.Gong W.Gradl S.Gramigna M.Greco M.H.Gu Y.T.Gu C.Y.Guan A.Q.Guo L.B.Guo M.J.Guo R.P.Guo Y.P.Guo A.Guskov J.Gutierrez K.L.Han T.T.Han F.Hanisch K.D.Hao X.Q.Hao F.A.Harris K.K.He K.L.He F.H.Heinsius C.H.Heinz Y.K.Heng C.Herold P.C.Hong G.Y.Hou X.T.Hou Y.R.Hou Z.L.Hou H.M.Hu J.F.Hu Q.P.Hu S.L.Hu T.Hu Y.Hu Z.M.Hu G.S.Huang K.X.Huang L.Q.Huang P.Huang X.T.Huang Y.P.Huang Y.S.Huang T.Hussain N.Hüsken N.in der Wiesche J.Jackson Q.Ji Q.P.Ji W.Ji X.B.Ji X.L.Ji Y.Y.Ji Z.K.Jia D.Jiang H.B.Jiang P.C.Jiang S.J.Jiang T.J.Jiang X.S.Jiang Y.Jiang J.B.Jiao J.K.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing X.M.Jing T.Johansson S.Kabana N.Kalantar-Nayestanaki X.L.Kang X.S.Kang M.Kavatsyuk B.C.Ke V.Khachatryan A.Khoukaz R.Kiuchi O.B.Kolcu B.Kopf M.Kuessner X.Kui N.Kumar A.Kupsc W.Kühn Q.Lan W.N.Lan T.T.Lei M.Lellmann T.Lenz C.Li C.Li C.Li C.H.Li C.K.Li D.M.Li F.Li G.Li H.B.Li H.J.Li H.N.Li Hui Li J.R.Li J.S.Li K.Li K.L.Li K.L.Li L.J.Li Lei Li M.H.Li M.R.Li P.L.Li P.R.Li Q.M.Li Q.X.Li R.Li S.X.Li T.Li T.Y.Li W.D.Li W.G.Li X.Li X.H.Li X.L.Li X.Y.Li X.Z.Li Y.Li Y.G.Li Y.P.Li Z.J.Li Z.Y.Li H.Liang Y.F.Liang Y.T.Liang G.R.Liao L.B.Liao M.H.Liao Y.P.Liao J.Libby A.Limphirat C.C.Lin D.X.Lin L.Q.Lin T.Lin B.J.Liu B.X.Liu c.liu C.X.Liu F.Liu F.H.Liu Feng Liu G.M.Liu H.Liu H.B.Liu H.H.Liu H.M.Liu Huihui Liu J.B.Liu J.J.Liu K.Liu K.Liu K.Y.Liu Ke Liu L.c.liu Lu Liu M.H.Liu P.L.Liu Q.Liu S.B.Liu T.Liu W.K.Liu W.M.Liu W.T.Liu X.Liu X.Liu X.K.Liu X.Y.Liu Y.Liu Y.Liu Y.Liu Y.B.Liu Z.A.Liu Z.D.Liu Z.Q.Liu X.C.Lou F.X.Lu H.J.Lu J.G.Lu X.L.Lu Y.Lu Y.H.Lu Y.P.Lu Z.H.Lu C.L.Luo J.R.Luo J.S.Luo M.X.Luo T.Luo X.L.Luo Z.Y.Lv X.R.Lyu Y.F.Lyu Y.H.Lyu F.C.Ma H.L.Ma J.L.Ma L.L.Ma L.R.Ma Q.M.Ma R.Q.Ma R.Y.Ma T.Ma X.T.Ma X.Y.Ma Y.M.Ma F.E.Maas I.MacKay M.Maggiora S.Malde Q.A.Malik H.X.Mao Y.J.Mao Z.P.Mao S.Marcello A.Marshall F.M.Melendi Y.H.Meng Z.X.Meng G.Mezzadri H.Miao T.J.Min R.E.Mitchell X.H.Mo B.Moses N.Yu.Muchnoi J.Muskalla Y.Nefedov F.Nerling L.S.Nie I.B.Nikolaev Z.Ning S.Nisar Q.L.Niu W.D.Niu C.Normand S.L.Olsen Q.Ouyang S.Pacetti X.Pan Y.Pan A.Pathak Y.P.Pei M.Pelizaeus H.P.Peng X.J.Peng Y.Y.Peng K.Peters K.Petridis J.L.Ping R.G.Ping S.Plura V.Prasad F.Z.Qi H.R.Qi M.Qi S.Qian W.B.Qian C.F.Qiao J.H.Qiao J.J.Qin J.L.Qin L.Q.Qin L.Y.Qin P.B.Qin X.P.Qin X.S.Qin Z.H.Qin J.F.Qiu Z.H.Qu J.Rademacker C.F.Redmer A.Rivetti M.Rolo G.Rong S.S.Rong F.Rosini Ch.Rosner M.Q.Ruan N.Salone A.Sarantsev Y.Schelhaas K.Schoenning M.Scodeggio K.Y.Shan W.Shan X.Y.Shan Z.J.Shang J.F.Shangguan L.G.Shao M.Shao C.P.Shen H.F.Shen W.H.Shen X.Y.Shen B.A.Shi H.Shi J.L.Shi J.Y.Shi S.Y.Shi X.Shi H.L.Song J.J.Song T.Z.Song W.M.Song Y.J.Song Y.X.Song S.Sosio S.Spataro F.Stieler S.S.Su Y.J.Su G.B.Sun G.X.Sun H.Sun H.K.Sun J.F.Sun K.Sun L.Sun S.S.Sun T.Sun Y.C.Sun Y.H.Sun Y.J.Sun Y.Z.Sun Z.Q.Sun Z.T.Sun C.J.Tang G.Y.Tang J.Tang J.J.Tang L.F.Tang Y.A.Tang L.Y.Tao M.Tat J.X.Teng J.Y.Tian W.H.Tian Y.Tian Z.F.Tian I.Uman B.Wang B.Wang Bo Wang C.Wang C.Wang Cong Wang D.Y.Wang H.J.Wang J.J.Wang K.Wang L.L.Wang L.W.Wang M.Wang M.Wang N.Y.Wang S.Wang T.Wang T.J.Wang W.Wang W.Wang W.P.Wang X.Wang X.F.Wang X.J.Wang X.L.Wang X.N.Wang Y.Wang Y.D.Wang Y.F.Wang Y.H.Wang Y.J.Wang Y.L.Wang Y.N.Wang Y.Q.Wang Yaqian Wang Yi Wang Yuan Wang Z.Wang Z.L.Wang Z.Q.Wang Z.Y.Wang D.H.Wei H.R.Wei F.Weidner S.P.Wen Y.R.Wen U.Wiedner G.Wilkinson M.Wolke C.Wu J.F.Wu L.H.Wu L.J.Wu Lianjie Wu S.G.Wu S.M.Wu X.Wu X.H.Wu Y.J.Wu Z.Wu L.Xia X.M.Xian B.H.Xiang D.Xiao G.Y.Xiao H.Xiao Y.L.Xiao Z.J.Xiao C.Xie K.J.Xie X.H.Xie Y.Xie Y.G.Xie Y.H.Xie Z.P.Xie T.Y.Xing C.F.Xu C.J.Xu G.F.Xu H.Y.Xu M.Xu Q.J.Xu Q.N.Xu T.D.Xu W.Xu W.L.Xu X.P.Xu Y.Xu Y.C.Xu Z.S.Xu F.Yan H.Y.Yan L.Yan W.B.Yan W.C.Yan W.H.Yan W.P.Yan X.Q.Yan H.J.Yang H.L.Yang H.X.Yang J.H.Yang R.J.Yang T.Yang Y.Yang Y.F.Yang Y.H.Yang Y.Q.Yang Y.X.Yang Y.Z.Yang M.Ye M.H.Ye Z.J.Ye Junhao Yin Z.Y.You B.X.Yu C.X.Yu G.Yu J.S.Yu L.Q.Yu M.C.Yu T.Yu X.D.Yu Y.C.Yu C.Z.Yuan H.Yuan J.Yuan J.Yuan L.Yuan S.C.Yuan X.Q.Yuan Y.Yuan Z.Y.Yuan C.X.Yue Ying Yue A.A.Zafar S.H.Zeng X.Zeng Y.Zeng Y.J.Zeng Y.J.Zeng X.Y.Zhai Y.H.Zhan A.Q.Zhang B.L.Zhang B.X.Zhang D.H.Zhang G.Y.Zhang G.Y.Zhang H.Zhang H.Zhang H.C.Zhang H.H.Zhang H.Q.Zhang H.R.Zhang H.Y.Zhang J.Zhang J.Zhang J.J.Zhang J.L.Zhang J.Q.Zhang J.S.Zhang J.W.Zhang J.X.Zhang J.Y.Zhang J.Z.Zhang Jianyu Zhang L.M.Zhang Lei Zhang N.Zhang P.Zhang Q.Zhang Q.Y.Zhang R.Y.Zhang S.H.Zhang Shulei Zhang X.M.Zhang X.Y Zhang X.Y.Zhang Y.Zhang Y.Zhang Y.T.Zhang Y.H.Zhang Y.M.Zhang Y.P.Zhang Z.D.Zhang Z.H.Zhang Z.L.Zhang Z.L.Zhang Z.X.Zhang Z.Y.Zhang Z.Y.Zhang Z.Z.Zhang Zh.Zh.Zhang G.Zhao J.Y.Zhao J.Z.Zhao L.Zhao L.Zhao M.G.Zhao N.Zhao R.P.Zhao S.J.Zhao Y.B.Zhao Y.L.Zhao Y.X.Zhao Z.G.Zhao A.Zhemchugov B.Zheng B.M.Zheng J.P.Zheng W.J.Zheng X.R.Zheng Y.H.Zheng B.Zhong C.Zhong H.Zhou J.Q.Zhou J.Y.Zhou S.Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou Y.X.Zhou Y.Z.Zhou A.N.Zhu J.Zhu K.Zhu K.J.Zhu K.S.Zhu L.Zhu L.X.Zhu S.H.Zhu T.J.Zhu W.D.Zhu W.D.Zhu W.J.Zhu W.Z.Zhu Y.C.Zhu Z.A.Zhu X.Y.Zhuang J.H.Zou J.Zu 《Chinese Physics C》 2025年第12期1-15,共15页
Based on a sample of 2.7x 10^(9)ψ(3686)events collected by the BESIII detector operating at the BEP-CII collider,the decay 4(3686)→YX_(cJ),X_(cJ)→ηηη’is analyzed.The decay modes X_(c1)and X_(c2)→ηηη’are ob... Based on a sample of 2.7x 10^(9)ψ(3686)events collected by the BESIII detector operating at the BEP-CII collider,the decay 4(3686)→YX_(cJ),X_(cJ)→ηηη’is analyzed.The decay modes X_(c1)and X_(c2)→ηηη’are observed for the first time,and their corresponding branching fractions are determined to be B(X_(c1)→ηηη’)=(1.40±0.13(stat.)±0.09(sys.))×10^(-4)and B(X_(c2)→ηηη’)=(4.18±0.84(stat.)±0.48(sys.))×10^(-5).An upper limit on the branching fraction of x_(co)→ηηη’is set as 2.59×10^(-5)at a 90%confidence level(CL).A partial wave analys-is(PWA)of the decay X_(c1)→ηηη’is performed to search for the 1^(-+)exotic stateη1(1855).The PWA result indic-ates that the structure in theηη’mass spectrum is attributed to f_(0)(1500),while in the m mass spectrum,it is attrib-uted to the 0^(++)phase space.The upper limit of B(x_(cl)→η1(1855)η)·B(η1(1855)→ηη')<9.79×10^(-5)is set based on the PWA at 90%CL. 展开更多
关键词 BESIII Hydron physics HYBRID
原文传递
Search for the lepton number violation decay ω→π^(+)π^(+)e^(-)e^(-)+c.c.
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作者 M.Ablikim M.N.Achasov +727 位作者 P.Adlarson X.C.Ai R.Aliberti A.Amoroso Q.An Y.Bai O.Bakina Y.Ban H.-R.Bao V.Batozskaya K.Begzsuren N.Berger M.Berlowski M.Bertani D.Bettoni A F.Bianchi E.Bianco A.Bortone I.Boyko R.A.Briere A.Brueggemann H.Cai M.H.Cai X.Cai A.Calcaterra G.F.Cao N.Cao S.A.Cetin X.Y.Chai J.F.Chang G.R.Che Y.Z.Che C.H.Chen Chao Chen G.Chen H.S.Chen H.Y.Chen M.L.Chen S.J.Chen S.L.Chen S.M.Chen T.Chen X.R.Chen X.T.Chen X.Y.Chen Y.B.Chen Y.Q.Chen Y.Q.Chen Z.Chen Z.J.Chen Z.K.Chen S.K.Choi X.Chu G.Cibinetto F.Cossio J.Cottee-Meldrum J.J.Cui H.L.Dai J.P.Dai A.Dbeyssi R.E.de Boer D.Dedovich C.Q.Deng Z.Y.Deng A.Denig I.Denysenko M.Destefanis F.De Mori B.Ding X.X.Ding Y.Ding Y.Ding Y.X.Ding J.Dong L.Y.Dong M.Y.Dong X.Dong M.C.Du S.X.Du S.X.Du Y.Y.Duan Z.H.Duan P.Egorov G.F.Fan J.J.Fan Y.H.Fan J.Fang J.Fang S.S.Fang W.X.Fang Y.Q.Fang R.Farinelli L.Fava F.Feldbauer G.Felici C.Q.Feng J.H.Feng L.Feng Q.X.Feng Y.T.Feng M.Fritsch C.D.Fu J.L.Fu Y.W.Fu H.Gao X.B.Gao Y.Gao Y.N.Gao Y.N.Gao Y.Y.Gao Z.Gao S.Garbolino I.Garzia L.Ge P.T.Ge Z.W.Ge C.Geng E.M.Gersabeck A.Gilman K.Goetzen J.D.Gong L.Gong W.X.Gong W.Gradl S.Gramigna M.Greco M.H.Gu Y.T.Gu C.Y.Guan A.Q.Guo L.B.Guo M.J.Guo R.P.Guo Y.P.Guo A.Guskov J.Gutierrez K.L.Han T.T.Han F.Hanisch K.D.Hao X.Q.Hao F.A.Harris K.K.He K.L.He F.H.Heinsius C.H.Heinz Y.K.Heng C.Herold P.C.Hong G.Y.Hou X.T.Hou Y.R.Hou Z.L.Hou H.M.Hu J.F.Hu Q.P.Hu S.L.Hu T.Hu Y.Hu Z.M.Hu G.S.Huang K.X.Huang L.Q.Huang P.Huang X.T.Huang Y.P.Huang Y.S.Huang T.Hussain N.Hüsken N.in der Wiesche J.Jackson Q.Ji Q.P.Ji W.Ji X.B.Ji X.L.Ji Y.Y.Ji Z.K.Jia D.Jiang H.B.Jiang P.C.Jiang S.J.Jiang T.J.Jiang X.S.Jiang Y.Jiang J.B.Jiao J.K.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing X.M.Jing T.Johansson S.Kabana N.Kalantar-Nayestanaki X.L.Kang X.S.Kang M.Kavatsyuk B.C.Ke V.Khachatryan A.Khoukaz R.Kiuchi O.B.Kolcu B.Kopf M.Kuessner X.Kui N.Kumar A.Kupsc W.Kühn Q.Lan W.N.Lan T.T.Lei M.Lellmann T.Lenz C.Li C.Li C.H.Li C.K.Li D.M.Li F.Li G.Li H.B.Li H.J.Li H.N.Li Hui Li J.R.Li J.S.Li K.Li K.L.Li K.L.Li L.J.Li Lei Li M.H.Li M.R.Li P.L.Li P.R.Li Q.M.Li Q.X.Li R.Li S.X.Li T.Li T.Y.Li W.D.Li W.G.Li X.Li X.H.Li X.L.Li X.Y.Li X.Z.Li Y.Li Y.G.Li Y.P.Li Z.J.Li Z.Y.Li C.Liang H.Liang Y.F.Liang Y.T.Liang G.R.Liao L.B.Liao M.H.Liao Y.P.Liao J.Libby A.Limphirat C.C.Lin D.X.Lin L.Q.Lin T.Lin B.J.Liu B.X.Liu c.liu C.X.Liu F.Liu F.H.Liu Feng Liu G.M.Liu H.Liu H.B.Liu H.H.Liu H.M.Liu Huihui Liu J.B.Liu J.J.Liu K.Liu K.Liu K.Y.Liu Ke Liu L.c.liu Lu Liu M.H.Liu M.H.Liu P.L.Liu Q.Liu S.B.Liu T.Liu W.K.Liu W.M.Liu W.T.Liu X.Liu X.Liu X.K.Liu X.L.Liu X.Y.Liu Y.Liu Y.Liu Y.Liu Y.B.Liu Z.A.Liu Z.D.Liu Z.Q.Liu X.C.Lou F.X.Lu H.J.Lu J.G.Lu X.L.Lu Y.Lu Y.H.Lu Y.P.Lu Z.H.Lu C.L.Luo J.R.Luo J.S.Luo M.X.Luo T.Luo X.L.Luo Z.Y.Lv X.R.Lyu Y.F.Lyu Y.H.Lyu F.C.Ma H.L.Ma Heng Ma J.L.Ma L.L.Ma L.R.Ma Q.M.Ma R.Q.Ma R.Y.Ma T.Ma X.T.Ma X.Y.Ma Y.M.Ma F.E.Maas I.MacKay M.Maggiora S.Malde Q.A.Malik H.X.Mao Y.J.Mao Z.P.Mao S.Marcello A.Marshall F.M.Melendi Y.H.Meng Z.X.Meng G.Mezzadri H.Miao T.J.Min R.E.Mitchell X.H.Mo B.Moses N.Yu.Muchnoi J.Muskalla Y.Nefedov F.Nerling L.S.Nie I.B.Nikolaev Z.Ning S.Nisar Q.L.Niu W.D.Niu C.Normand S.L.Olsen Q.Ouyang S.Pacetti X.Pan Y.Pan A.Pathak Y.P.Pei M.Pelizaeus H.P.Peng X.J.Peng Y.Y.Peng K.Peters K.Petridis J.L.Ping R.G.Ping S.Plura V.Prasad F.Z.Qi H.R.Qi M.Qi S.Qian W.B.Qian C.F.Qiao J.H.Qiao J.J.Qin J.L.Qin L.Q.Qin L.Y.Qin P.B.Qin X.P.Qin X.S.Qin Z.H.Qin J.F.Qiu Z.H.Qu J.Rademacker C.F.Redmer A.Rivetti M.Rolo G.Rong S.S.Rong F.Rosini Ch.Rosner M.Q.Ruan N.Salone A.Sarantsev Y.Schelhaas K.Schoenning M.Scodeggio K.Y.Shan W.Shan X.Y.Shan Z.J.Shang J.F.Shangguan L.G.Shao M.Shao C.P.Shen H.F.Shen W.H.Shen X.Y.Shen B.A.Shi H.Shi J.L.Shi J.Y.Shi S.Y.Shi X.Shi H.L.Song J.J.Song T.Z.Song W.M.Song Y.J.Song Y.X.Song Zirong Song S.Sosio S.Spataro F.Stieler S.S Su Y.J.Su G.B.Sun G.X.Sun H.Sun H.K.Sun J.F.Sun K.Sun L.Sun S.S.Sun T.Sun Y.C.Sun Y.H.Sun Y.J.Sun Y.Z.Sun Z.Q.Sun Z.T.Sun C.J.Tang G.Y.Tang J.Tang J.J.Tang L.F.Tang Y.A.Tang L.Y.Tao M.Tat J.X.Teng J.Y.Tian W.H.Tian Y.Tian Z.F.Tian I.Uman B.Wang B.Wang Bo Wang C.Wang C.Wang Cong Wang D.Y.Wang H.J.Wang J.J.Wang K.Wang L.L.Wang L.W.Wang M.Wang M.Wang N.Y.Wang S.Wang T.Wang T.J.Wang W.Wang W.Wang W.P.Wang X.Wang X.F.Wang X.J.Wang X.L.Wang X.N.Wang Y.Wang Y.D.Wang Y.F.Wang Y.H.Wang Y.J.Wang Y.L.Wang Y.N.Wang Y.Q.Wang Yaqian Wang Yi Wang Yuan Wang Z.Wang Z.L.Wang Z.L.Wang Z.Q.Wang Z.Y.Wang D.H.Wei H.R.Wei F.Weidner S.P.Wen Y.R.Wen U.Wiedner G.Wilkinson M.Wolke C.Wu J.F.Wu L.H.Wu L.J.Wu L.J.Wu Lianjie Wu S.G.Wu S.M.Wu X.Wu X.H.Wu Y.J.Wu Z.Wu L.Xia X.M.Xian B.H.Xiang D.Xiao G.Y.Xiao H.Xiao Y.L.Xiao Z.J.Xiao C.Xie K.J.Xie X.H.Xie Y.Xie Y.G.Xie Y.H.Xie Z.P.Xie T.Y.Xing C.F.Xu C.J.Xu G.F.Xu H.Y.Xu H.Y.Xu M.Xu Q.J.Xu Q.N.Xu T.D.Xu W.Xu W.L.Xu X.P.Xu Y.Xu Y.Xu Y.C.Xu Z.S.Xu F.Yan H.Y.Yan L.Yan W.B.Yan W.C.Yan W.H.Yan W.P.Yan X.Q.Yan H.J.Yang H.L.Yang H.X.Yang J.H.Yang R.J.Yang T.Yang Y.Yang Y.F.Yang Y.H.Yang Y.Q.Yang Y.X.Yang Y.Z.Yang M.Ye M.H.Ye Z.J.Ye Junhao Yin Z.Y.You B.X.Yu C.X.Yu G.Yu J.S.Yu L.Q.Yu M.C.Yu T.Yu X.D.Yu Y.C.Yu C.Z.Yuan H.Yuan J.Yuan J.Yuan L.Yuan S.C.Yuan X.Q.Yuan Y.Yuan Z.Y.Yuan C.X.Yue Ying Yue A.A.Zafar S.H.Zeng X.Zeng Y.Zeng Y.J.Zeng Y.J.Zeng X.Y.Zhai Y.H.Zhan Zhang A.Q.Zhang B.L.Zhang B.X.Zhang D.H.Zhang G.Y.Zhang G.Y.Zhang H.Zhang H.Zhang H.C.Zhang H.H.Zhang H.Q.Zhang H.R.Zhang H.Y.Zhang J.Zhang J.Zhang J.J.Zhang J.L.Zhang J.Q.Zhang J.S.Zhang J.W.Zhang J.X.Zhang J.Y.Zhang J.Z.Zhang Jianyu Zhang L.M.Zhang Lei Zhang N.Zhang P.Zhang Q.Zhang Q.Y.Zhang R.Y.Zhang S.H.Zhang Shulei Zhang X.M.Zhang X.Y Zhang X.Y.Zhang Y.Zhang Y.Zhang Y.T.Zhang Y.H.Zhang Y.M.Zhang Y.P.Zhang Z.D.Zhang Z.H.Zhang Z.L.Zhang Z.L.Zhang Z.X.Zhang Z.Y.Zhang Z.Y.Zhang Z.Z.Zhang Zh.Zh.Zhang G.Zhao J.Y.Zhao J.Z.Zhao L.Zhao L.Zhao M.G.Zhao N.Zhao R.P.Zhao S.J.Zhao Y.B.Zhao Y.L.Zhao Y.X.Zhao Z.G.Zhao A.Zhemchugov B.Zheng B.M.Zheng J.P.Zheng W.J.Zheng X.R.Zheng Y.H.Zheng B.Zhong C.Zhong H.Zhou J.Q.Zhou J.Y.Zhou S.Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou Y.X.Zhou Y.Z.Zhou A.N.Zhu J.Zhu K.Zhu K.J.Zhu K.S.Zhu L.Zhu L.X.Zhu S.H.Zhu T.J.Zhu W.D.Zhu W.D.Zhu W.J.Zhu W.Z.Zhu Y.C.Zhu Z.A.Zhu X.Y.Zhuang J.H.Zou J.Zu BESIII Collaboration 《Chinese Physics C》 2025年第10期15-24,共10页
Lepton number violation decayω→π^(+)π^(+)e^(-)e^(-)+c.c.is searched for via J/ψ→ωηusing a data sample of(1.0087±0.0044)×10^(10)J/ψevents collected via the BESIII detector at the BEPCII collider.No s... Lepton number violation decayω→π^(+)π^(+)e^(-)e^(-)+c.c.is searched for via J/ψ→ωηusing a data sample of(1.0087±0.0044)×10^(10)J/ψevents collected via the BESIII detector at the BEPCII collider.No significant signal is observed,and the upper limit on the branching fraction ofω→π^(+)π^(+)e^(-)e^(-)+c.c.at the 90%confidence level is determined for the first time to be 2.8×10^(-6). 展开更多
关键词 lepton number violation matter anti-matter asymmetry neutrinoless double beta decay
原文传递
Search for the leptonic decay D^(+)→e^(+)ν_(e)
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作者 M.Ablikim M.N.Achasov +668 位作者 P.Adlarson O.Afedulidis X.C.Ai R.Aliberti A.Amoroso Q.An Y.Bai O.Bakina I.Balossino Y.Ban H.-R.Bao V.Batozskaya K.Begzsuren N.Berger M.Berlowski M.Bertani D.Bettoni F.Bianchi E.Bianco A.Bortone I.Boyko R.A.Briere A.Brueggemann H.Cai X.Cai A.Calcaterra G.F.Cao N.Cao S.A.Cetin X.Y.Chai J.F.Chang G.R.Che Y.Z.Che G.Chelkov C.Chen C.H.Chen Chao Chen G.Chen H.S.Chen H.Y.Chen M.L.Chen S.J.Chen S.L.Chen S.M.Chen T.Chen X.R.Chen X.T.Chen Y.B.Chen Y.Q.Chen Z.J.Chen Z.Y.Chen S.K.Choi G.Cibinetto F.Cossio J.J.Cui H.L.Dai J.P.Dai A.Dbeyssi R.E.de Boer D.Dedovich C.Q.Deng Z.Y.Deng A.Denig I.Denysenko M.Destefanis F.De Mori B.Ding X.X.Ding Y.Ding Y.Ding J.Dong L.Y.Dong M.Y.Dong X.Dong M.C.Du S.X.Du Y.Y.Duan Z.H.Duan P.Egorov Y.H.Fan J.Fang J.Fang S.S.Fang W.X.Fang Y.Fang Y.Q.Fang R.Farinelli L.Fava F.Feldbauer G.Felici C.Q.Feng J.H.Feng Y.T.Feng M.Fritsch C.D.Fu J.L.Fu Y.W.Fu H.Gao X.B.Gao Y.N.Gao Yang Gao S.Garbolino I.Garzia L.Ge P.T.Ge Z.W.Ge C.Geng E.M.Gersabeck A.Gilman K.Goetzen L.Gong W.X.Gong W.Gradl S.Gramigna M.Greco M.H.Gu Y.T.Gu C.Y.Guan A.Q.Guo L.B.Guo M.J.Guo R.P.Guo Y.P.Guo A.Guskov J.Gutierrez K.L.Han T.T.Han F.Hanisch X.Q.Hao F.A.Harris K.K.He K.L.He F.H.Heinsius C.H.Heinz Y.K.Heng C.Herold T.Holtmann P.C.Hong G.Y.Hou X.T.Hou Y.R.Hou Z.L.Hou B.Y.Hu H.M.Hu J.F.Hu S.L.Hu T.Hu Y.Hu G.S.Huang K.X.Huang L.Q.Huang X.T.Huang Y.P.Huang Y.S.Huang T.Hussain F.Hölzken N.Hüsken N.in der Wiesche J.Jackson S.Janchiv J.H.Jeong Q.Ji Q.P.Ji W.Ji X.B.Ji X.L.Ji Y.Y.Ji X.Q.Jia Z.K.Jia D.Jiang H.B.Jiang P.C.Jiang S.S.Jiang T.J.Jiang X.S.Jiang Y.Jiang J.B.Jiao J.K.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing X.M.Jing T.Johansson S.Kabana N.Kalantar-Nayestanaki X.L.Kang X.S.Kang M.Kavatsyuk B.C.Ke V.Khachatryan A.Khoukaz R.Kiuchi O.B.Kolcu B.Kopf M.Kuessner X.Kui N.Kumar A.Kupsc W.Kühn J.J.Lane L.Lavezzi T.T.Lei Z.H.Lei M.Lellmann T.Lenz C.Li C.Li C.H.Li Cheng Li D.M.Li F.Li G.Li H.B.Li H.J.Li H.N.Li Hui Li J.R.Li J.S.Li K.Li K.L.Li L.J.Li L.K.Li Lei Li M.H.Li P.R.Li Q.M.Li Q.X.Li R.Li S.X.Li T.Li W.D.Li W.G.Li X.Li X.H.Li X.L.Li X.Y.Li X.Z.Li Y.G.Li Z.J.Li Z.Y.Li C.Liang H.Liang H.Liang Y.F.Liang Y.T.Liang G.R.Liao Y.P.Liao J.Libby A.Limphirat C.C.Lin D.X.Lin T.Lin B.J.Liu B.X.Liu c.liu C.X.Liu F.Liu F.H.Liu Feng Liu G.M.Liu H.Liu H.B.Liu H.H.Liu H.M.Liu Huihui Liu J.B.Liu J.Y.Liu K.Liu K.Y.Liu Ke Liu L.Liu L.c.liu Lu Liu M.H.Liu P.L.Liu Q.Liu S.B.Liu T.Liu W.K.Liu W.M.Liu X.Liu X.Liu Y.Liu Y.Liu Y.B.Liu Z.A.Liu Z.D.Liu Z.Q.Liu X.C.Lou F.X.Lu H.J.Lu J.G.Lu X.L.Lu Y.Lu Y.P.Lu Z.H.Lu C.L.Luo J.R.Luo M.X.Luo T.Luo X.L.Luo X.R.Lyu Y.F.Lyu F.C.Ma H.Ma H.L.Ma J.L.Ma L.L.Ma L.R.Ma M.M.Ma Q.M.Ma R.Q.Ma T.Ma X.T.Ma X.Y.Ma Y.M.Ma F.E.Maas I.MacKay M.Maggiora S.Malde Y.J.Mao Z.P.Mao S.Marcello Z.X.Meng J.G.Messchendorp G.Mezzadri H.Miao T.J.Min R.E.Mitchell X.H.Mo B.Moses N.Yu.Muchnoi J.Muskalla Y.Nefedov F.Nerling L.S.Nie I.B.Nikolaev Z.Ning S.Nisar Q.L.Niu W.D.Niu Y.Niu S.L.Olsen S.L.Olsen Q.Ouyang S.Pacetti X.Pan Y.Pan A.Pathak Y.P.Pei M.Pelizaeus H.P.Peng Y.Y.Peng K.Peters J.L.Ping R.G.Ping S.Plura V.Prasad F.Z.Qi H.Qi H.R.Qi M.Qi T.Y.Qi S.Qian W.B.Qian C.F.Qiao X.K.Qiao J.J.Qin L.Q.Qin L.Y.Qin X.P.Qin X.S.Qin Z.H.Qin J.F.Qiu Z.H.Qu C.F.Redmer K.J.Ren A.Rivetti M.Rolo G.Rong Ch.Rosner M.Q.Ruan S.N.Ruan N.Salone A.Sarantsev Y.Schelhaas K.Schoenning M.Scodeggio K.Y.Shan W.Shan X.Y.Shan Z.J.Shang J.F.Shangguan L.G.Shao M.Shao C.P.Shen H.F.Shen W.H.Shen X.Y.Shen B.A.Shi H.Shi H.C.Shi J.L.Shi J.Y.Shi Q.Q.Shi S.Y.Shi X.Shi J.J.Song T.Z.Song W.M.Song Y.J.Song Y.X.Song S.Sosio S.Spataro F.Stieler S.S Su Y.J.Su G.B.Sun G.X.Sun H.Sun H.K.Sun J.F.Sun K.Sun L.Sun S.S.Sun T.Sun W.Y.Sun Y.Sun Y.J.Sun Y.Z.Sun Z.Q.Sun Z.T.Sun C.J.Tang G.Y.Tang J.Tang M.Tang Y.A.Tang L.Y.Tao Q.T.Tao M.Tat J.X.Teng V.Thoren W.H.Tian Y.Tian Z.F.Tian I.Uman Y.Wan S.J.Wang B.Wang B.L.Wang Bo Wang D.Y.Wang F.Wang H.J.Wang J.J.Wang J.P.Wang K.Wang L.L.Wang M.Wang N.Y.Wang S.Wang S.Wang T.Wang T.J.Wang W.Wang W.Wang W.P.Wang X.Wang X.F.Wang X.J.Wang X.L.Wang X.N.Wang Y.Wang Y.D.Wang Y.F.Wang Y.L.Wang Y.N.Wang Y.Q.Wang Yaqian Wang Yi Wang Z.Wang Z.L.Wang Z.Y.Wang Ziyi Wang D.H.Wei F.Weidner S.P.Wen Y.R.Wen U.Wiedner G.Wilkinson M.Wolke L.Wollenberg C.Wu J.F.Wu L.H.Wu L.J.Wu X.Wu X.H.Wu Y.Wu Y.H.Wu Y.J.Wu Z.Wu L.Xia X.M.Xian B.H.Xiang T.Xiang D.Xiao G.Y.Xiao S.Y.Xiao Y.L.Xiao Z.J.Xiao C.Xie X.H.Xie Y.Xie Y.G.Xie Y.H.Xie Z.P.Xie T.Y.Xing C.F.Xu C.J.Xu G.F.Xu H.Y.Xu M.Xu Q.J.Xu Q.N.Xu W.Xu W.L.Xu X.P.Xu Y.Xu Y.C.Xu Z.S.Xu F.Yan L.Yan W.B.Yan W.C.Yan X.Q.Yan H.J.Yang H.L.Yang H.X.Yang T.Yang Y.Yang Y.F.Yang Y.F.Yang Y.X.Yang Z.W.Yang Z.P.Yao M.Ye M.H.Ye J.H.Yin Junhao Yin Z.Y.You B.X.Yu C.X.Yu G.Yu J.S.Yu M.C.Yu T.Yu X.D.Yu Y.C.Yu C.Z.Yuan J.Yuan J.Yuan L.Yuan S.C.Yuan Y.Yuan Z.Y.Yuan C.X.Yue A.A.Zafar F.R.Zeng S.H.Zeng X.Zeng Y.Zeng Y.J.Zeng Y.J.Zeng X.Y.Zhai Y.C.Zhai Y.H.Zhan A.Q.Zhang B.L.Zhang B.X.Zhang D.H.Zhang G.Y.Zhang H.Zhang H.Zhang H.C.Zhang H.H.Zhang H.H.Zhang H.Q.Zhang H.R.Zhang H.Y.Zhang J.Zhang J.Zhang J.J.Zhang J.L.Zhang J.Q.Zhang J.S.Zhang J.W.Zhang J.X.Zhang J.Y.Zhang J.Z.Zhang Jianyu Zhang L.M.Zhang Lei Zhang N.Zhang P.Zhang Q.Y.Zhang R.Y.Zhang S.H.Zhang Shulei Zhang X.M.Zhang X.Y Zhang X.Y.Zhang Y.Zhang Y.Zhang Y.T.Zhang Y.H.Zhang Y.M.Zhang Yan Zhang Z.D.Zhang Z.H.Zhang Z.L.Zhang Z.Y.Zhang Z.Y.Zhang Z.Z.Zhang G.Zhao J.Y.Zhao J.Z.Zhao L.Zhao Lei Zhao M.G.Zhao N.Zhao R.P.Zhao S.J.Zhao Y.B.Zhao Y.X.Zhao Z.G.Zhao A.Zhemchugov B.Zheng B.M.Zheng J.P.Zheng W.J.Zheng Y.H.Zheng B.Zhong X.Zhong H.Zhou J.Y.Zhou L.P.Zhou S.Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou Y.Z.Zhou Z.C.Zhou A.N.Zhu J.Zhu K.Zhu K.J.Zhu K.S.Zhu L.Zhu L.X.Zhu S.H.Zhu T.J.Zhu W.D.Zhu Y.C.Zhu Z.A.Zhu J.H.Zou J.Zu 《Chinese Physics C》 2025年第6期1-10,共10页
We search for the leptonic decay D^(+)→e^(+)ν_(e)using an e+e-collision data sample with an integrated luminosity of 20.3 fb-1collected with the BESIII detector at a center-of-mass energy of 3.773 GeV.Significant si... We search for the leptonic decay D^(+)→e^(+)ν_(e)using an e+e-collision data sample with an integrated luminosity of 20.3 fb-1collected with the BESIII detector at a center-of-mass energy of 3.773 GeV.Significant signal is not observed,and an upper limit on the branching fraction of D^(+)→e^(+)ν_(e)is set as 9.7×10^(-7),at a confidence level of 90%.Our upper limit is an order of magnitude smaller than the previous limit for this decay mode. 展开更多
关键词 BESII charm physics leptonic decay
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Search for Cabibbo-suppressed decays Λ_(c)^(+)→Σ^(0)K^(+)π^(0) and Λ_(c)^(+)→Σ^(0)K^(+)π^(+)π^(−)
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作者 M.Ablikim M.N.Achasov +691 位作者 P.Adlarson X.C.Ai R.Aliberti A.Amoroso Q.An Y.Bai O.Bakina Y.Ban H.-R.Bao V.Batozskaya K.Begzsuren N.Berger M.Berlowski M.Bertani D.Bettoni F.Bianchi E.Bianco A.Bortone I.Boyko R.A.Briere A.Brueggemann H.Cai M.H.Cai X.Cai A.Calcaterra G.F.Cao N.Cao S.A.Cetin X.Y.Chai J.F.Chang G.R.Che Y.Z.Che G.Chelkov C.Chen C.H.Chen Chao Chen G.Chen H.S.Chen H.Y.Chen M.L.Chen S.J.Chen S.L.Chen S.M.Chen T.Chen X.R.Chen X.T.Chen Y.B.Chen Y.Q.Chen Z.J.Chen Z.K.Chen S.K.Choi X.Chu G.Cibinetto F.Cossio J.J.Cui H.L.Dai J.P.Dai A.Dbeyssi R.E.de Boer D.Dedovich C.Q.Deng Z.Y.Deng A.Denig I.Denysenko M.Destefanis F.De Mori B.Ding X.X.Ding Y.Ding Y.Ding Y.X.Ding J.Dong L.Y.Dong M.Y.Dong X.Dong M.C.Du S.X.Du Y.Y.Duan Z.H.Duan P.Egorov G.F.Fan J.J.Fan Y.H.Fan J.Fang J.Fang S.S.Fang W.X.Fang Y.Q.Fang R.Farinelli L.Fava F.Feldbauer G.Felici C.Q.Feng J.H.Feng Y.T.Feng M.Fritsch C.D.Fu J.L.Fu Y.W.Fu H.Gao X.B.Gao Y.N.Gao Y.N.Gao Y.Y.Gao Yang Gao S.Garbolino I.Garzia P.T.Ge Z.W.Ge C.Geng E.M.Gersabeck A.Gilman K.Goetzen L.Gong W.X.Gong W.Gradl S.Gramigna M.Greco M.H.Gu Y.T.Gu C.Y.Guan A.Q.Guo L.B.Guo M.J.Guo R.P.Guo Y.P.Guo A.Guskov J.Gutierrez K.L.Han T.T.Han F.Hanisch K.D.Hao X.Q.Hao F.A.Harris K.K.He K.L.He F.H.Heinsius C.H.Heinz Y.K.Heng C.Herold T.Holtmann P.C.Hong G.Y.Hou X.T.Hou Y.R.Hou Z.L.Hou B.Y.Hu H.M.Hu J.F.Hu Q.P.Hu S.L.Hu T.Hu Y.Hu Z.M.Hu G.S.Huang K.X.Huang L.Q.Huang P.Huang X.T.Huang Y.P.Huang Y.S.Huang T.Hussain N.Hüsken N.in der Wiesche J.Jackson S.Janchiv Q.Ji Q.P.Ji W.Ji X.B.Ji X.L.Ji Y.Y.Ji Z.K.Jia D.Jiang H.B.Jiang P.C.Jiang S.J.Jiang T.J.Jiang X.S.Jiang Y.Jiang J.B.Jiao J.K.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing X.M.Jing T.Johansson S.Kabana N.Kalantar-Nayestanaki X.L.Kang X.S.Kang M.Kavatsyuk B.C.Ke V.Khachatryan A.Khoukaz R.Kiuchi O.B.Kolcu B.Kopf M.Kuessner X.Kui N.Kumar A.Kupsc W.Kühn Q.Lan W.N.Lan T.T.Lei Z.H.Lei M.Lellmann T.Lenz C.Li C.Li C.H.Li C.K.Li Cheng Li D.M.Li F.Li G.Li H.B.Li H.J.Li H.N.Li Hui Li J.R.Li J.S.Li K.Li K.L.Li K.L.Li L.J.Li Lei Li M.H.Li M.R.Li P.L.Li P.R.Li Q.M.Li Q.X.Li R.Li T.Li T.Y.Li W.D.Li W.G.Li X.Li X.H.Li X.L.Li X.Y.Li X.Z.Li Y.Li Y.G.Li Z.J.Li Z.Y.Li C.Liang H.Liang Y.F.Liang Y.T.Liang G.R.Liao L.B.Liao M.H.Liao Y.P.Liao J.Libby A.Limphirat C.C.Lin C.X.Lin D.X.Lin L.Q.Lin T.Lin B.J.Liu B.X.Liu c.liu C.X.Liu F.Liu F.H.Liu Feng Liu G.M.Liu H.Liu H.B.Liu H.H.Liu H.M.Liu Huihui Liu J.B.Liu J.J.Liu K.Liu K.Liu K.Y.Liu Ke Liu L.Liu L.c.liu Lu Liu M.H.Liu P.L.Liu Q.Liu S.B.Liu T.Liu W.K.Liu W.M.Liu W.T.Liu X.Liu X.Liu X.Y.Liu Y.Liu Y.Liu Y.Liu Y.B.Liu Z.A.Liu Z.D.Liu Z.Q.Liu X.C.Lou F.X.Lu H.J.Lu J.G.Lu Y.Lu Y.H.Lu Y.P.Lu Z.H.Lu C.L.Luo J.R.Luo J.S.Luo M.X.Luo T.Luo X.L.Luo X.R.Lyu Y.F.Lyu Y.H.Lyu F.C.Ma H.Ma H.L.Ma J.L.Ma L.L.Ma L.R.Ma Q.M.Ma R.Q.Ma R.Y.Ma T.Ma X.T.Ma X.Y.Ma Y.M.Ma F.E.Maas I.MacKay M.Maggiora S.Malde Y.J.Mao Z.P.Mao S.Marcello Y.H.Meng Z.X.Meng J.G.Messchendorp G.Mezzadri H.Miao T.J.Min R.E.Mitchell X.H.Mo B.Moses N.Yu.Muchnoi J.Muskalla Y.Nefedov F.Nerling L.S.Nie I.B.Nikolaev Z.Ning S.Nisar Q.L.Niu S.L.Olsen Q.Ouyang S.Pacetti X.Pan Y.Pan A.Pathak Y.P.Pei M.Pelizaeus H.P.Peng Y.Y.Peng K.Peters e J.L.Ping R.G.Ping S.Plura V.Prasad F.Z.Qi H.R.Qi M.Qi S.Qian W.B.Qian C.F.Qiao J.H.Qiao J.J.Qin J.L.Qin L.Q.Qin L.Y.Qin P.B.Qin X.P.Qin X.S.Qin Z.H.Qin J.F.Qiu Z.H.Qu C.F.Redmer A.Rivetti M.Rolo G.Rong S.S.Rong Ch.Rosner M.Q.Ruan S.N.Ruan N.Salone A.Sarantsev Y.Schelhaas K.Schoenning M.Scodeggio K.Y.Shan W.Shan X.Y.Shan Z.J.Shang J.F.Shangguan L.G.Shao M.Shao C.P.Shen H.F.Shen W.H.Shen X.Y.Shen B.A.Shi H.Shi J.L.Shi J.Y.Shi S.Y.Shi X.Shi H.L.Song J.J.Song T.Z.Song W.M.Song Y.J.Song Y.X.Song S.Sosio S.Spataro F.Stieler S.S Su Y.J.Su G.B.Sun G.X.Sun H.Sun H.K.Sun J.F.Sun K.Sun L.Sun S.S.Sun T.Sun Y.C.Sun Y.H.Sun Y.J.Sun Y.Z.Sun Z.Q.Sun Z.T.Sun C.J.Tang G.Y.Tang J.Tang L.F.Tang M.Tang Y.A.Tang L.Y.Tao M.Tat J.X.Teng V.Thoren J.Y.Tian W.H.Tian Y.Tian Z.F.Tian I.Uman B.Wang B.Wang Bo Wang C.Wang D.Y.Wang H.J.Wang J.J.Wang K.Wang L.L.Wang L.W.Wang M.Wang M.Wang N.Y.Wang S.Wang S.Wang T.Wang T.J.Wang W.Wang W.Wang W.P.Wang X.Wang X.F.Wang X.J.Wang X.L.Wang X.N.Wang Y.Wang Y.D.Wang Y.F.Wang Y.H.Wang Y.L.Wang Y.N.Wang Y.Q.Wang Yaqian Wang Yi Wang Yuan Wang Z.Wang Z.L.Wang Z.Y.Wang D.H.Wei F.Weidner S.P.Wen Y.R.Wen U.Wiedner G.Wilkinson M.Wolke C.Wu J.F.Wu L.H.Wu L.J.Wu Lianjie Wu S.G.Wu S.M.Wu X.Wu X.H.Wu Y.J.Wu Z.Wu L.Xia X.M.Xian B.H.Xiang T.Xiang D.Xiao G.Y.Xiao H.Xiao Y.L.Xiao Z.J.Xiao C.Xie K.J.Xie X.H.Xie Y.Xie Y.G.Xie Y.H.Xie Z.P.Xie T.Y.Xing C.F.Xu C.J.Xu G.F.Xu M.Xu Q.J.Xu Q.N.Xu W.L.Xu X.P.Xu Y.Xu Y.C.Xu Z.S.Xu F.Yan H.Y.Yan L.Yan W.B.Yan W.C.Yan W.P.Yan X.Q.Yan H.J.Yang f H.L.Yang H.X.Yang J.H.Yang R.J.Yang T.Yang Y.Yang Y.F.Yang Y.Q.Yang Y.X.Yang Y.Z.Yang M.Ye M.H.Ye Junhao Yin Z.Y.You B.X.Yu C.X.Yu G.Yu J.S.Yu M.C.Yu T.Yu X.D.Yu Y.C.Yu C.Z.Yuan H.Yuan J.Yuan J.Yuan L.Yuan S.C.Yuan Y.Yuan Z.Y.Yuan C.X.Yue Ying Yue A.A.Zafar S.H.Zeng X.Zeng Y.Zeng Y.J.Zeng Y.J.Zeng X.Y.Zhai Y.H.Zhan A.Q.Zhang B.L.Zhang B.X.Zhang D.H.Zhang G.Y.Zhang G.Y.Zhang H.Zhang H.Zhang H.C.Zhang H.H.Zhang H.Q.Zhang H.R.Zhang H.Y.Zhang J.Zhang J.Zhang J.J.Zhang J.L.Zhang J.Q.Zhang J.S.Zhang J.W.Zhang J.X.Zhang J.Y.Zhang J.Z.Zhang Jianyu Zhang L.M.Zhang Lei Zhang N.Zhang P.Zhang Q.Zhang Q.Y.Zhang R.Y.Zhang S.H.Zhang Shulei Zhang X.M.Zhang X.Y Zhang X.Y.Zhang Y.Zhang Y.Zhang Y.T.Zhang Y.H.Zhang Y.M.Zhang Z.D.Zhang Z.H.Zhang Z.L.Zhang Z.L.Zhang Z.X.Zhang Z.Y.Zhang Z.Y.Zhang Z.Z.Zhang Zh.Zh.Zhang G.Zhao J.Y.Zhao J.Z.Zhao L.Zhao Lei Zhao M.G.Zhao N.Zhao R.P.Zhao S.J.Zhao Y.B.Zhao Y.L.Zhao Y.X.Zhao Z.G.Zhao A.Zhemchugov B.Zheng B.M.Zheng J.P.Zheng W.J.Zheng X.R.Zheng Y.H.Zheng B.Zhong X.Zhong H.Zhou J.Y.Zhou S.Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou Y.Z.Zhou Z.C.Zhou A.N.Zhu J.Zhu K.Zhu K.J.Zhu K.S.Zhu L.Zhu L.X.Zhu S.H.Zhu T.J.Zhu W.D.Zhu W.J.Zhu W.Z.Zhu Y.C.Zhu Z.A.Zhu X.Y.Zhuang J.H.Zou J.Zu 《Chinese Physics C》 2025年第7期14-26,共13页
Utilizing 4.5 fb^(-1)ofe^(+)e^(-)annihilation data collected at center-of-mass energies ranging from 4599.53 MeV to 4698.82 MeV by the BESIII detector at the BEPCII collider,we searched for singly Cabibbo-suppressed h... Utilizing 4.5 fb^(-1)ofe^(+)e^(-)annihilation data collected at center-of-mass energies ranging from 4599.53 MeV to 4698.82 MeV by the BESIII detector at the BEPCII collider,we searched for singly Cabibbo-suppressed hadronic decaysΛ_(c)^(+)→Σ^(0)K^(+)π^(0)andΛ_(c)^(+)→Σ^(0)K^(+)π^(+)π^(−)and with a single-tag method.No significant signals were observed for both decays.The upper limits on the branching fractions at the 90%confidence level were determined to be 5.0×10^(-4)for and forΛ_(c)^(+)→Σ^(0)K^(+)π^(0)and 6.5×10^(-4)forΛ_(c)^(+)→Σ^(0)K^(+)π^(+)π^(−). 展开更多
关键词 Charmed baryon SCS decay BESIII Experiment
原文传递
Observation of the Crab Nebula with LHAASO-KM2A−a performance study 被引量:12
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作者 F.Aharonian Q.An +245 位作者 Axikegu L.X.Bai Y.X.Bai Y.W.Bao D.Bastieri X.J.Bi Y.J.Bi H.Cai J.T.Cai Z.Cao J.Chang J.F.Chang X.C.Chang B.M.Chen J.Chen L.Chen M.J.Chen M.L.Chen Q.H.Chen S.H.Chen S.Z.Chen T.L.Chen X.L.Chen Y.Chen N.Cheng Y.D.Cheng S.W.Cui X.H.Cui Y.D.Cui B.Z.Dai H.L.Dai Z.G.Dai D.della Volpe B.D'Ettorre Piazzoli X.J.Dong J.H.Fan Y.Z.Fan Z.X.Fan J.Fang K.Fang C.F.Feng L.Feng S.H.Feng Y.L.Feng B.Gao C.D.Gao Q.Gao W.Gao M.M.Ge L.S.Geng G.H.Gong Q.B.Gou M.H.Gu J.G.Guo X.L.Guo Y.Q.Guo Y.Y.Guo Y.A.Han H.H.He H.N.He J.C.He S.L.He X.B.He Y.He M.Heller Y.K.Hor C.Hou X.Hou H.B.Hu S.Hu S.C.Hu X.J.Hu D.H.Huang Q.L.Huang W.H.Huang X.T.Huang Z.C.Huang F.Ji X.L.Ji H.Y.Jia K.Jiang Z.J.Jiang C.Jin D.Kuleshov K.Levochkin B.B.Li C.Li F.Li H.B.Li H.C.Li H.Y.Li J.Li K.Li W.L.Li X.Li X.R.Li Y.Li Y.Z.Li Z.Li E.W.Liang Y.F.Liang S.J.Lin B.Liu c.liu D.Liu H.Liu H.D.Liu J.Liu J.L.Liu J.S.Liu J.Y.Liu M.Y.Liu R.Y.Liu S.M.Liu W.Liu Y.N.Liu Z.X.Liu W.J.Long R.Lu H.K.Lv B.Q.Ma L.L.Ma X.H.Ma J.R.Mao A.Masood W.Mitthumsiri T.Montaruli Y.C.Nan B.Y.Pang P.Pattarakijwanich Z.Y.Pei M.Y.Qi D.Ruffolo V.Rulev A.Sáiz L.Shao O.Shchegolev X.D.Sheng J.R.Shi H.C.Song Yu.V.Stenkin V.Stepanov Q.N.Sun X.N.Sun Z.B.Sun P.H.T.Tam Z.B.Tang W.W.Tian B.D.Wang C.Wang H.Wang H.G.Wang J.C.Wang J.S.Wang L.P.Wang L.Y.Wang R.N.Wang W.Wang X.G.Wang X.J.Wang X.Y.Wang Y.D.Wang Y.J.Wang Y.P.Wang Z.Wang Z.H.Wang Z.X.Wang D.M.Wei J.J.Wei Y.J.Wei T.Wen C.Y.Wu H.R.Wu S.Wu W.X.Wu X.F.Wu S.Q.Xi J.Xia J.J.Xia G.M.Xiang G.Xiao H.B.Xiao G.G.Xin Y.L.Xin Y.Xing D.L.Xu R.X.Xu L.Xue D.H.Yan C.W.Yang F.F.Yang J.Y.Yang L.L.Yang M.J.Yang R.Z.Yang S.B.Yang Y.H.Yao Z.G.Yao Y.M.Ye L.Q.Yin N.Yin X.H.You Z.Y.You Y.H.Yu Q.Yuan H.D.Zeng T.X.Zeng W.Zeng Z.K.Zeng M.Zha X.X.Zhai B.B.Zhang H.M.Zhang H.Y.Zhang J.L.Zhang J.W.Zhang L.Zhang L.X.Zhang P.F.Zhang P.P.Zhang R.Zhang S.R.Zhang S.S.Zhang X.Zhang X.P.Zhang Y.Zhang Y.F.Zhang Y.L.Zhang B.Zhao J.Zhao L.Zhao L.Z.Zhao S.P.Zhao F.Zheng Y.Zheng B.Zhou H.Zhou J.N.Zhou P.Zhou R.Zhou X.X.Zhou C.G.Zhu F.R.Zhu H.Zhu K.J.Zhu X.Zuo 《Chinese Physics C》 SCIE CAS CSCD 2021年第2期518-530,共13页
A sub-array of the Large High Altitude Air Shower Observatory(LHAASO),KM2A is mainly designed to observe a large fraction of the northern sky to hunt for γ-ray sources at energies above 10 TeV.Even though the detecto... A sub-array of the Large High Altitude Air Shower Observatory(LHAASO),KM2A is mainly designed to observe a large fraction of the northern sky to hunt for γ-ray sources at energies above 10 TeV.Even though the detector construction is still underway,half of the KM2A array has been operating stably since the end of 2019.In this paper,we present the KM2A data analysis pipeline and the first observation of the Crab Nebula,a standard candle in very high energy γ-ray astronomy.We detect γ-ray signals from the Crab Nebula in both energy ranges of 10-100 TeV and>100 TeV with high significance,by analyzing the KM2A data of 136 live days between December 2019 and May 2020.With the observations,we test the detector performance,including angular resolution,pointing accuracy and cosmic-ray background rejection power.The energy spectrum of the Crab Nebula in the energy range 10-250 TeV fits well with a single power-law function dN/dE=(1.13±0.05stat±0.08sys)×10^(-14).(E/20 TeV)-309±0.06stat±0.02syscm^(-2) s^(-1) TeV^(-1).It is consistent with previous measurements by other experiments.This opens a new window of γ-ray astronomy above 0.1 PeV through which new ultrahigh-energy γ-ray phenomena,such as cosmic PeVatrons,might be discovered. 展开更多
关键词 Γ-RAY Crab Nebula extensive air showers cosmic rays
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Performance of LHAASO-WCDA and observation of the Crab Nebula as a standard candle 被引量:5
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作者 F.Aharonian Q.An +257 位作者 Axikegu L.X.Bai Y.X.Bai Y.W.Bao D.Bastieri X.J.Bi Y.J.Bi H.Cai J.T.Cai Z.Cao Z.Cao J.Chang J.F.Chang X.C.Chang B.M.Chen J.Chen L.Chen L.Chen L.Chen M.J.Chen M.L.Chen Q.H.Chen S.H.Chen S.Z.Chen T.L.Chen X.L.Chen Y.Chen N.Cheng Y.D.Cheng S.W.Cui X.H.Cui Y.D.Cui B.Z.Dai H.L.Dai Z.G.Dai Danzengluobu D.della Volpe B.D'Ettorre Piazzoli X.J.Dong J.H.Fan Y.Z.Fan Z.X.Fan J.Fang K.Fang C.F.Feng L.Feng S.H.Feng Y.L.Feng B.Gao C.D.Gao Q.Gao W.Gao M.M.Ge L.S.Geng G.H.Gong Q.B.Gou M.H.Gu J.G.Guo X.L.Guo Y.Q.Guo Y.Y.Guo Y.A.Han H.H.He H.N.He J.C.He S.L.He X.B.He Y.He M.Heller Y.K.Hor C.Hou X.Hou H.B.Hu S.Hu S.C.Hu X.J.Hu D.H.Huang Q.L.Huang W.H.Huang X.T.Huang Z.C.Huang F.Ji X.L.Ji H.Y.Jia K.Jiang Z.J.Jiang C.Jin D.Kuleshov K.Levochkin B.B.Li C.Li C.Li F.Li H.B.Li H.C.Li H.Y.Li J.Li K.Li W.L.Li X.Li X.Li X.R.Li Y.Li Y.Z.Li Z.Li Z.Li E.W.Liang Y.F.Liang S.J.Lin B.Liu c.liu D.Liu H.Liu H.D.Liu J.Liu J.L.Liu J.S.Liu J.Y.Liu M.Y.Liu R.Y.Liu S.M.Liu W.Liu Y.N.Liu Z.X.Liu W.J.Long R.Lu H.K.Lv B.Q.Ma L.L.Ma X.H.Ma J.R.Mao A.Masood W.Mitthumsiri T.Montaruli Y.C.Nan B.Y.Pang P.Pattarakijwanich Z.Y.Pei M.Y.Qi B.Q.Qiao D.Ruffolo V.Rulev A.Saiz L.Shao O.Shchegolev X.D.Sheng J.R.Shi H.C.Song Yu.V.Stenkin V.Stepanov Q.N.Sun X.N.Sun Z.B.Sun P.H.T.Tam Z.B.Tang W.W.Tian B.D.Wang C.Wang H.Wang H.G.Wang J.C.Wang J.S.Wang L.P.Wang L.Y.Wang R.N.Wang W.Wang W.Wang X.G.Wang X.J.Wang X.Y.Wang Y.D.Wang Y.J.Wang Y.P.Wang Z.Wang Z.Wang Z.H.Wang Z.X.Wang D.M.Wei J.J.Wei Y.J.Wei T.Wen C.Y.Wu H.R.Wu S.Wu W.X.Wu X.F.Wu S.Q.Xi J.Xia J.J.Xia G.M.Xiang G.Xiao H.B.Xiao G.G.Xin Y.L.Xin Y.Xing D.L.Xu R.X.Xu L.Xue D.H.Yan C.W.Yang F.F.Yang J.Y.Yang L.L.Yang M.J.Yang R.Z.Yang S.B.Yang Y.H.Yao Z.G.Yao Y.M.Ye L.Q.Yin N.Yin X.H.You Z.Y.You Y.H.Yu Q.Yuan H.D.Zeng T.X.Zeng W.Zeng Z.K.Zeng M.Zha X.X.Zhai B.B.Zhang H.M.Zhang H.Y.Zhang J.L.Zhang J.W.Zhang L.Zhang L.Zhang L.X.Zhang P.F.Zhang P.P.Zhang R.Zhang S.R.Zhang S.S.Zhang X.Zhang X.P.Zhang Y.Zhang Y.Zhang Y.F.Zhang Y.L.Zhang B.Zhao J.Zhao L.Zhao L.Z.Zhao S.P.Zhao F.Zheng Y.Zheng B.Zhou H.Zhou J.N.Zhou P.Zhou R.Zhou X.X.Zhou C.G.Zhu F.R.Zhu H.Zhu K.J.Zhu X.Zuo 《Chinese Physics C》 SCIE CAS CSCD 2021年第8期166-181,共16页
The first Water Cherenkov detector of the LHAASO experiment(WCDA-1)has been operating since April 2019.The data for the first year have been analyzed to test its performance by observing the Crab Nebula as a standard ... The first Water Cherenkov detector of the LHAASO experiment(WCDA-1)has been operating since April 2019.The data for the first year have been analyzed to test its performance by observing the Crab Nebula as a standard candle.The WCDA-1 achieves a sensitivity of 65 mCU per year,with a statistical threshold of 5 cr.To accomplish this,a 97.7%cosmic-ray background rejection rate around 1 TeV and 99.8%around 6 TeV with an ap proximate photon acceptance of 50%is achieved after applying an algorithm to separate gamma-induced showers.The angular resolution is measured using the Crab Nebula as a point source to be approximately 0.45°at 1 TeV and better than 0.2°above 6 TeV,with a pointing accuracy better than 0.05°.These values all match the design specifications.The energy resolution is found to be 33%for gamma rays around 6 TeV.The spectral energy distribution of the Crab Nebula in the range from 500 GeV to 15.8 TeV is measured and found to be in agreement with the results from other TeV gamma ray observatories. 展开更多
关键词 LHAASO-WCDA Crab Nebula angular resolution spectral energy distribution
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