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Behavioral Intention to Continue Using a Library Mobile App
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作者 X.Zhang h.liu +2 位作者 Z.h.liu J.R.Ming Y.Zhou 《Computer Systems Science & Engineering》 SCIE EI 2023年第7期357-369,共13页
To meet the needs of today’s library users,institutions are developing library mobile apps(LMAs),as their libraries are increasingly intelligent and rely on deep learning.This paper explores the influencing factors a... To meet the needs of today’s library users,institutions are developing library mobile apps(LMAs),as their libraries are increasingly intelligent and rely on deep learning.This paper explores the influencing factors and differences in the perception of LMAs at different time points after a user has downloaded an LMA.A research model was constructed based on the technology acceptance model.A questionnaire was designed and distributed twice to LMA users with an interval of three months to collect dynamic data.The analysis was based on structural equation modeling.The empirical results show that the perceived ease of use,the perceived usefulness,the social influence,and the facilitating conditions affected the users’behavioral intention,but their impacts were different at different times.As the usage time increases,the technology acceptance model is still universal for understanding the user perception of LMA.In addition,two extended variables(social impact and convenience)also affect the user’s behavior intention.User behavior is dynamic and changed over time.This study is important both theoretically and practically,as the results could be used to improve the service quality of LMAs and reduce the loss rate of users.Its findings may help the designers and developers of LMAs to optimize them from the perspective of a user and improve the service experience by providing a deeper understanding of the adoption behavior of information systems by LMA users. 展开更多
关键词 Library mobile app user perception behavioral intention technology acceptance model information system adoption
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急性病毒性肝炎的诊疗 被引量:3
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作者 王豪 J.Heathcote +7 位作者 A.Elewaut S.Fedail A.Gangl S.Hamid M.Shah D.Lavanchy h.liu J.Krabshuis 《胃肠病学和肝病学杂志》 CAS 2004年第2期116-123,共8页
关键词 急性病毒性肝炎 诊断 治疗 自限性疾病
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Computational aerodynamics of low Reynolds number plunging,pitching and flexible wings for MAV applications 被引量:15
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作者 W.Shyy Y.Lian +7 位作者 J.Tang h.liu P.Trizila B.Stanford L.Bernal C.Cesnik P.Friedmann P.Ifju 《Acta Mechanica Sinica》 SCIE EI CAS CSCD 2008年第4期351-373,共23页
Micro air vehicles (MAV's) have the potential to revolutionize our sensing and information gathering capabilities in environmental monitoring and homeland security areas. Due to the MAV's' small size, flight regi... Micro air vehicles (MAV's) have the potential to revolutionize our sensing and information gathering capabilities in environmental monitoring and homeland security areas. Due to the MAV's' small size, flight regime, and modes of operation, significant scientific advancement will be needed to create this revolutionary capability. Aerodynamics, structural dynamics, and flight dynamics of natural flyers intersects with some of the richest problems in MAV's, inclu- ding massively unsteady three-dimensional separation, transition in boundary layers and shear layers, vortical flows and bluff body flows, unsteady flight environment, aeroelasticity, and nonlinear and adaptive control are just a few examples. A challenge is that the scaling of both fluid dynamics and structural dynamics between smaller natural flyer and practical flying hardware/lab experiment (larger dimension) is fundamentally difficult. In this paper, we offer an overview of the challenges and issues, along with sample results illustrating some of the efforts made from a computational modeling angle. 展开更多
关键词 Micro air vehicles AERODYNAMICS Flexible wings Low Reynolds number
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Methods for a blind analysis of isobar data collected by the STAR collaboration 被引量:7
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作者 J.Adam L.Adamczyk +366 位作者 J.R.Adams J.K.Adkins G.Agakishiev M.M.Aggarwal Z.Ahammed I.Alekseev D.M.Anderson A.Aparin E.C.Aschenauer M.U.Ashraf F.G.Atetalla A.Attri G.S.Averichev V.Bairathi K.Barish A.Behera R.Bellwied A.Bhasin J.Bielcik J.Bielcikova L.C.Bland I.G.Bordyuzhin J.D.Brandenburg A.V.Brandin J.Butterworth H.Caines M.Calderon de la Barca Sanchez D.Cebra I.Chakaberia P.Chaloupka B.K.Chan F-H.Chang Z.Chang N.Chankova-Bunzarova A.Chatterjee D.Chen J.Chen J.H.Chen X.Chen Z.Chen J.Cheng M.Cherney M.Chevalier S.Choudhury W.Christie X.Chu H.J.Crawford M.Csanad M.Daugherity T.G.Dedovich I.M.Deppner A.A.Derevschikov L.Didenko X.Dong J.L.Drachenberg J.C.Dunlop T.Edmonds N.Elsey J.Engelage G.Eppley S.Esumi O.Evdokimov A.Ewigleben O.Eyser R.Fatemi S.Fazio P.Federic J.Fedorisin C.J.Feng Y.Feng P.Filip E.Finch Y.Fisyak A.Francisco L.Fulek C.A.Gagliardi T.Galatyuk F.Geurts A.Gibson K.Gopal X.Gou D.Grosnick W.Guryn A.I.Hamad A.Hamed S.Harabasz J.W.Harris S.He W.He X.H.He Y.He S.Heppelmann S.Heppelmann N.Herrmann E.Hoffman L.Holub Y.Hong S.Horvat Y.Hu H.Z.Huang S.L.Huang T.Huang X.Huang T.J.Humanic P.Huo G.Igo D.Isenhower W.W.Jacobs C.Jena A.Jentsch Y.Ji J.Jia K.Jiang S.Jowzaee X.Ju E.G.Judd S.Kabana M.L.Kabir S.Kagamaster D.Kalinkin K.Kang D.Kapukchyan K.Kauder H.W.Ke D.Keane A.Kechechyan M.Kelsey Y.V.Khyzhniak D.P.Kikoła C.Kim B.Kimelman D.Kincses T.A.Kinghorn I.Kisel A.Kiselev M.Kocan L.Kochenda L.K.Kosarzewski L.Kramarik P.Kravtsov K.Krueger N.Kulathunga Mudiyanselage L.Kumar S.Kumar R.Kunnawalkam Elayavalli J.H.Kwasizur R.Lacey S.Lan J.M.Landgraf J.Lauret A.Lebedev R.Lednicky J.H.Lee Y.H.Leung C.Li C.Li W.Li W.Li X.Li Y.Li Y.Liang R.Licenik T.Lin Y.Lin M.A.Lisa F.Liu h.liu P.Liu P.Liu T.Liu X.Liu Y.Liu Z.Liu T.Ljubicic W.J.Llope R.S.Longacre N.S.Lukow S.Luo X.Luo G.L.Ma L.Ma R.Ma Y.G.Ma N.Magdy R.Majka D.Mallick S.Margetis C.Markert H.S.Matis J.A.Mazer N.G.Minaev S.Mioduszewski B.Mohanty I.Mooney Z.Moravcova D.A.Morozov M.Nagy J.D.Nam Md.Nasim K.Nayak D.Neff J.M.Nelson D.B.Nemes M.Nie G.Nigmatkulov T.Niida L.V.Nogach T.Nonaka A.S.Nunes G.Odyniec A.Ogawa S.Oh V.A.Okorokov B.S.Page R.Pak A.Pandav Y.Panebratsev B.Pawlik D.Pawlowska H.Pei C.Perkins L.Pinsky R.L.Pinter J.Pluta J.Porter M.Posik N.K.Pruthi M.Przybycien J.Putschke H.Qiu A.Quintero S.K.Radhakrishnan S.Ramachandran R.L.Ray R.Reed H.G.Ritter O.V.Rogachevskiy J.L.Romero L.Ruan J.Rusnak N.R.Sahoo H.Sako S.Salur J.Sandweiss S.Sato W.B.Schmidke N.Schmitz B.R.Schweid F.Seck J.Seger M.Sergeeva R.Seto P.Seyboth N.Shah E.Shahaliev P.V.Shanmuganathan M.Shao A.I.Sheikh W.Q.Shen S.S.Shi Y.Shi Q.Y.Shou E.P.Sichtermann R.Sikora M.Simko J.Singh S.Singha N.Smirnov W.Solyst P.Sorensen H.M.Spinka B.Srivastava T.D.S.Stanislaus M.Stefaniak D.J.Stewart M.Strikhanov B.Stringfellow A.A.P.Suaide M.Sumbera B.Summa X.M.Sun X.Sun Y.Sun Y.Sun B.Surrow D.N.Svirida P.Szymanski A.H.Tang Z.Tang A.Taranenko T.Tarnowsky J.H.Thomas A.R.Timmins D.Tlusty M.Tokarev C.A.Tomkiel S.Trentalange R.E.Tribble P.Tribedy S.K.Tripathy O.D.Tsai Z.Tu T.Ullrich D.G.Underwood I.Upsal G.Van Buren J.Vanek A.N.Vasiliev I.Vassiliev F.Videbæk S.Vokal S.A.Voloshin F.Wang G.Wang J.S.Wang P.Wang Y.Wang Y.Wang Z.Wang J.C.Webb P.C.Weidenkaff L.Wen G.D.Westfall H.Wieman S.W.Wissink R.Witt Y.Wu Z.G.Xiao G.Xie W.Xie H.Xu N.Xu Q.H.Xu Y.F.Xu Y.Xu Z.Xu Z.Xu C.Yang Q.Yang S.Yang Y.Yang Z.Yang Z.Ye Z.Ye L.Yi K.Yip Y.Yu H.Zbroszczyk W.Zha C.Zhang D.Zhang S.Zhang S.Zhang X.P.Zhang Y.Zhang Y.Zhang Z.J.Zhang Z.Zhang Z.Zhang J.Zhao C.Zhong C.Zhou X.Zhu Z.Zhu M.Zurek M.Zyzak STAR Collaboration Abilene 《Nuclear Science and Techniques》 SCIE EI CAS CSCD 2021年第5期43-50,共8页
In 2018,the STAR collaboration collected data from^(96)_(44)Ru+^(96)_(44)Ru and^(96)_(40)Zr+^(96)_(40)Zr at√^(S)NN=200 Ge V to search for the presence of the chiral magnetic effect in collisions of nuclei.The isobar ... In 2018,the STAR collaboration collected data from^(96)_(44)Ru+^(96)_(44)Ru and^(96)_(40)Zr+^(96)_(40)Zr at√^(S)NN=200 Ge V to search for the presence of the chiral magnetic effect in collisions of nuclei.The isobar collision species alternated frequently between 9644 Ru+^(96)_(44)Ru and^(96)_(40)Zr+^(96)_(40)Zr.In order to conduct blind analyses of studies related to the chiral magnetic effect in these isobar data,STAR developed a three-step blind analysis procedure.Analysts are initially provided a"reference sample"of data,comprised of a mix of events from the two species,the order of which respects time-dependent changes in run conditions.After tuning analysis codes and performing time-dependent quality assurance on the reference sample,analysts are provided a species-blind sample suitable for calculating efficiencies and corrections for individual≈30-min data-taking runs.For this sample,species-specific information is disguised,but individual output files contain data from a single isobar species.Only run-by-run corrections and code alteration subsequent to these corrections are allowed at this stage.Following these modifications,the"frozen"code is passed over the fully un-blind data,completing the blind analysis.As a check of the feasibility of the blind analysis procedure,analysts completed a"mock data challenge,"analyzing data from Au+Au collisions at√^(S)NN=27 Ge V,collected in 2018.The Au+Au data were prepared in the same manner intended for the isobar blind data.The details of the blind analysis procedure and results from the mock data challenge are presented. 展开更多
关键词 Blind analysis Chiral magnetic effect Heavy-ion collisions
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Power Balance Estimation in Long Duration Discharges on QUEST 被引量:1
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作者 K.HANADA H.ZUSHI +18 位作者 H.IDEI K.NAKAMURA M.ISHIGURO S.TASHIMA E.I.KALINNIKOVA Y.NAGASHIMA M.HASEGAWA A.FUJISAWA A.HIGASHIJIMA S.KAWASAKI H.NAKASHIMA O.MITARAI A.FUKUYAMA Y.TAKASE X.GAO h.liu J.QIAN M.ONO R.RAMAN 《Plasma Science and Technology》 SCIE EI CAS CSCD 2016年第11期1069-1075,共7页
Fully non-inductive plasma start-up was successfully achieved by using a well- controlled microwave source on the spherical tokamak, QUEST. Non-inductive plasmas were maintained for approximately 3-5 min, during which... Fully non-inductive plasma start-up was successfully achieved by using a well- controlled microwave source on the spherical tokamak, QUEST. Non-inductive plasmas were maintained for approximately 3-5 min, during which time power balance estimates could be achieved by monitoring wall and cooling-water temperatures. Approximately 70%-90% of the injected power could be accounted for by calorimetric measurements and approximately half of the injected power was found to be deposited on the vessel wall, which is slightly dependent on the magnetic configuration. The power distribution to water-cooled limiters, which are expected to be exposed to local heat loads, depends significantly on the magnetic configuration, however some of the deposited power is due to energetic electrons, which have large poloidal orbits and are likely to be deposited on the plasma facing components. 展开更多
关键词 steady state operation spherical tokamak plasma wall interaction power balance
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血浆粉、乳糖和不同来源大豆蛋白对断奶仔猪生产性能的影响
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作者 h.liu 王仁华 《饲料广角》 2016年第18期36-41,共6页
本试验共有371头断奶仔猪用于评定血浆粉(SDP)、不同来源的大豆蛋白和乳糖对断奶仔猪生产性能的影响.在试验1中,128头断奶仔猪(5.99kg,18±2d)在2×2×2因素设计被用于评定第Ι阶段(0~14d)日粮中血浆粉(0 VS 7%)、乳糖(0 VS... 本试验共有371头断奶仔猪用于评定血浆粉(SDP)、不同来源的大豆蛋白和乳糖对断奶仔猪生产性能的影响.在试验1中,128头断奶仔猪(5.99kg,18±2d)在2×2×2因素设计被用于评定第Ι阶段(0~14d)日粮中血浆粉(0 VS 7%)、乳糖(0 VS 3%)和两种不同来源大豆蛋白[大豆粉(SBM)和豆粕(ESPC)]对断奶仔猪生产性能的影响.试验结果表明:在含大豆粉的日粮中,血浆粉可提高第Ι阶段平均日增重(ADG)(P<0.01)和日平均采食量(ADFI)(P<0.05).但在含豆粕的日粮中,血浆粉则作用不明显.乳糖可提高第Ι阶段ADG和肉料比(G/F)(P<0.01).在试验2中,144头断奶仔猪(5.50kg,17±3d)在2×3×2因素设计被用于评定第Ι阶段(0~14d)日粮中血浆粉(0 VS3.5%)和三种不同来源大豆蛋白[大豆粉(SBM)、豆粕(ESPC)和大豆蛋白粉(SPC)]和第Ⅱ阶段两种日粮(简单日粮VS复合日粮)对断奶仔猪生产性能的影响.在第Ι阶段,血浆粉可增加ADG(P<0.01)和G/F(P<0.05).断奶仔猪采食大豆粉后,获得最高的ADG和ADFI,并且在肉料比(G/F)上,类似饲喂豆粕后的效果.在第Ⅱ阶段,与采食简单日粮相比,断奶仔猪采食复合日粮更能提高ADG(P<0.01)、ADFI(P<0.05)和肉料比(G/F)(P<0.05).在试验3中,99头断奶仔猪(5.77kg,17±3d)被用于评定第Ι阶段(0~14d)日粮中大豆粉、豆粕与血浆粉混合物对断奶仔猪生产性能的影响.试验表明,断奶仔猪采食大豆粉(不含血制品)日粮后,在第Ι 阶段的第一个星期ADG(P<0.01)、ADFI(P<0.01)和G/F(P<0.05)等生产性能达到最低水平.不同来源的大豆蛋白在第Ι阶段日粮中对断奶仔猪的生产性能的影响不明显.这些试验表明血浆粉和乳糖可提高第Ι阶段断奶仔猪的生产性能,在第Ι阶段日粮中,大豆粉和血浆粉可作为断奶仔猪主要的蛋白质来源. 展开更多
关键词 断奶仔猪 不同来源 豆粕 乳糖含量 生产性能 ADG 采食量 大豆粉 日粮类型 大豆蛋白
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Effects of generally anisotropic crustal rocks on fault-induced displacement and strain fields
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作者 E.Pan W.A.Griffith h.liu 《Geodesy and Geodynamics》 2019年第5期394-401,共8页
We present a new solution for the elastic displacement and strain fields on or near Earth’s surface due to rectangular faults in an anisotropic half-space,expressed as a summation of(A)the solution in an infinite spa... We present a new solution for the elastic displacement and strain fields on or near Earth’s surface due to rectangular faults in an anisotropic half-space,expressed as a summation of(A)the solution in an infinite space which is singular,and(B)the complementary part which is regular and well-behaved.These two solutions are expressed in terms of the mathematically elegant and computationally powerful Stroh formalism and can be applied to the generally anisotropic rock half-space or a transversely isotropic rock mass with any oriented plane of isotropy.For any flat fault of polygonal shape,one needs only to carry out a simple line integral from 0 to 7 r in order to express the fault-induced response.Numerical examples are presented to demonstrate the significant effect of the rock anisotropy and layer orientation on the fault-induced displacement and strain fields in anisotropic rocks.Potential applications are wide ranging,from faults in sedimentary strata to strongly deformed metamorphic rocks with steeply dipping foliation. 展开更多
关键词 GEOMECHANICS Rock ANISOTROPY BEDDING plane Deformation and strain FIELDS Mechanics theory and modelling
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Observation of inhomogeneity in congruent LiTaO3 crystal
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作者 X.B.Hu H.D.Jiang +5 位作者 h.liu S.S.Jiang Q.Li J.Y.Wang C.Q.Zhang B.Ten 《Beijing Synchrotron Radiation Facility》 2001年第2期142-144, ,共3页
The inhomogeneity in a congrunet LiTaO3 crystal has been observed by transmission synchrotron topography.Many extraordinary regions exist in congruent LiTaO3 crystal and they often show diffraction intensity different... The inhomogeneity in a congrunet LiTaO3 crystal has been observed by transmission synchrotron topography.Many extraordinary regions exist in congruent LiTaO3 crystal and they often show diffraction intensity different from that of ordinary regions in synchrotron topographs.Differential thermal analysis indiates that the Curie temperature of the extraordinary region is lower than that of ordinary region,and the extraordinary region is really a high defect density region.The diffraction contrast of the extraordinary region in synchrotron topographs is explained qualitatively by a calculation at the selected wavelength.2001 Published by Elsevier Science B.V. 展开更多
关键词 LITAO3晶体 钽酸锂晶体 同步辐射形貌术 结构分析 X射线分析
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Rational design of AgGaS/ZnS/ZnS quantum dots with a near-unity photoluminescence quantum yield via double shelling scheme
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作者 H.X.Lu h.liu +5 位作者 Z.Z.Fu Y.Y.Chen H.Q.Dai Z.Hu W.L.Zhang R.Q.Guo 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2024年第2期235-242,共8页
In this study,a two-step method was used to synthesize highly luminescent AgGaS/ZnS/ZnS quantum dots(QDs).In the first step,an inner ZnS shell was formed via a one-pot method,which resulted in a smaller lattice mismat... In this study,a two-step method was used to synthesize highly luminescent AgGaS/ZnS/ZnS quantum dots(QDs).In the first step,an inner ZnS shell was formed via a one-pot method,which resulted in a smaller lattice mismatch between the AgGaS core and the outer ZnS shell,thereby facilitating the formation of a thick outer shell.After the two-step shelling process,the synthesized AgGaS/ZnS/ZnS QDs showed an excellent photoluminescence quantum yield(PLQY)of 96.4%with a peak wavelength of 508 nm,repre-senting the highest PLQY reported thus far for AgGaS QDs.Furthermore,the effect of halogen ions in Zn precursors on the shelling process was investigated.It was proposed that the capacity of halogen ions to coordinate with the QDs influenced the balance between Zn cation diffusion and ZnS shelling reaction.Specifically,the ZnS shelling reaction was dominant when ZnCl_(2)was employed,while Zn cation diffusion was the dominant process under the I^(−)-rich environment.This work provides insights into the interfacial restructuring during the ZnS shelling and offers a clear map for the tailored synthesis of core/shell QDs. 展开更多
关键词 AgGaS Quantum dots PHOTOLUMINESCENCE Core/shell Alloyed core/shell interface
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Evidence for particle acceleration approaching PeV energies in the W51 complex
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作者 LHAASO Collaboration Zhen Cao +287 位作者 F.Aharonian 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.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 L.S.Geng G.Giacinti G.H.Gong Q.B.Gou M.H.Gu F.L.Guo X.L.Guo Y.Q.Guo Y.Y.Guo Y.A.Han 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 D.H.Huang T.Q.Huang W.J.Huang X.T.Huang X.Y.Huang Y.Huang X.L.Ji H.Y.Jia K.Jia K.Jiang X.W.Jiang Z.J.Jiang M.Jin M.M.Kang I.Karpikov 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 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.Sáiz 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 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 S.Celli 《Science Bulletin》 SCIE EI CAS CSCD 2024年第18期2833-2841,共9页
Theγ-ray emission from the W51 complex is widely acknowledged to be attributed to the interaction between the cosmic rays(CRs)accelerated by the shock of supernova remnant(SNR)W51C and the dense molecular clouds in t... Theγ-ray emission from the W51 complex is widely acknowledged to be attributed to the interaction between the cosmic rays(CRs)accelerated by the shock of supernova remnant(SNR)W51C and the dense molecular clouds in the adjacent star-forming region,W51B.However,the maximum acceleration capability of W51C for CRs remains elusive.Based on observations conducted with the Large High Altitude Air Shower Observatory(LHAASO),we report a significant detection ofγrays emanating from the W51 complex,with energies from 2 to 200 TeV.The LHAASO measurements,for the first time,extend theγ-ray emission from the W51 complex beyond 100 TeV and reveal a significant spectrum bending at tens of TeV.By combining the"π^(0)-decay bump"featured data from Fermi-LAT,the broadbandγ-ray spectrum of the W51 region can be well-characterized by a simple pp-collision model.The observed spectral bending feature suggests an exponential cutoff at~400 TeV or a power-law break at~200 TeV in the CR proton spectrum,most likely providing the first evidence of SNRs serving as CR accelerators approaching the PeV regime.Additionally,two young star clusters within W51B could also be theoretically viable to produce the most energeticγrays observed by LHAASO.Our findings strongly support the presence of extreme CR accelerators within the W51 complex and provide new insights into the origin of Galactic CRs. 展开更多
关键词 UHE c-ray Cosmic rays SNR W51C Star clusters
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Amplitude analysis of the decays D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)
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作者 M.Ablikim M.N.Achasov +642 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 J.F.Chang W.L.Chang G.R.Che G.Chelkov C.Chen C.H.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 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.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 K.Fischer M.Fritsch C.D.Fu J.L.Fu Y.W.Fu H.Gao Y.N.Gao Yang Gao S.Garbolino I.Garzia P.T.Ge Z.W.Ge C.Geng E.M.Gersabeck 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 JA.Gilman K.Goetzen L.Gong W.X.Gong W.Gradl S.Gramigna M.Greco M.H.Gu Y.T.Gu C.Y.Guan Z.L.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 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.H\"olzken N.H\"usken N.in der Wiesche M.Irshad 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 A.Kupsc W.K\"uhn J.J.Lane P.Larin L.Lavezzi T.T.Lei Z.H.Lei H.Leithoff M.Lellmann T.Lenz C.Li C.Li C.H.Li Cheng Li D.M.Li F.Li G.Li H.Li H.B.Li H.J.Li H.N.Li Hui Li J.R.Li J.S.Li K.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 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 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 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.T.Ma X.Y.Ma 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 A.Pathak 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 J.J.Qin L.Q.Qin X.S.Qin Z.H.Qin J.F.Qiu S.Q.Qu Z.H.Qu C.F.Redmer K.J.Ren A.Rivetti M.Rolo G.Rong Ch.Rosner 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.C.Shi J.L.Shi J.Y.Shi Q.Q.Shi R.S.Shi S.Y.Shi X.Shi X.D.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.Q.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 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.P.Wang K.Wang L.L.Wang M.Wang Meng 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.Wei 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 Q.J.Xu Q.N.Xu W.Xu W.L.Xu X.P.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 C.Z.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.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.M.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 H.Zhou J.Y.Zhou L.P.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 W.D.Zhu Y.C.Zhu Z.A.Zhu J.H.Zou J.Zu 《Chinese Physics C》 SCIE CAS CSCD 2024年第8期6-33,共28页
Using e^(+)e^(−)annihilation data corresponding to an integrated luminosity of 2.93 fb^(−1)taken at the center-of-mass energy√s=3.773 GeV with the BESIII detector,a joint amplitude analysis is performed on the decays... Using e^(+)e^(−)annihilation data corresponding to an integrated luminosity of 2.93 fb^(−1)taken at the center-of-mass energy√s=3.773 GeV with the BESIII detector,a joint amplitude analysis is performed on the decays D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η).The fit fractions of individual components are obtained,and large interferences among the dominant components of the decays D^(0)→a_(1)(1260)π,D^(0)→π(1300)π,D^(0)→ρ(770)ρ(770),and D^(0)→2(ππ)_(S)are observed in both channels.With the obtained amplitude model,the CP-even fractions of D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η)are determined to be(75.2±1.1_(stat).±1.5_(syst.))%and(68.9±1.5_(stat).±2.4_(syst.))%,respectively.The branching fractions of D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η)are measured to be(0.688±0.010_(stat.)±0.010_(syst.))%and(0.951±0.025_(stat.)±0.021_(syst.))%,respectively.The amplitude analysis provides an important model for the binning strategy in measuring the strong phase parameters of D^(0)→4πwhen used to determine the CKM angleγ(ϕ_(3))via the B^(−)→DK^(−)decay. 展开更多
关键词 BESIII D^(0)meson decays amplitude analysis CP-even fraction
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Determination of the number ofψ(3686)events taken at BESⅢ
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作者 M.Ablikim M.N.Achasov +660 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 J.F.Chang G.R.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 Z.L.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 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 P.Larin 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 Ke 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.Z.Li Xiaoyu Li Y.G.Li Z.J.Li Z.X.Li Z.Y.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 C.C.Lin D.X.Lin T.Lin B.J.Liu B.X.Liu C.Liu C.X.Liu F.h.liu Fang Liu Feng Liu G.M.Liu h.liu H.B.Liu H.M.Liu Huanhuan 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 M.M.Ma Q.M.Ma R.Q.Ma T.Ma X.T.Ma X.Y.Ma Y.Ma Y.M.Ma F.E.Maas 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 Q.Ouyang S.Pacetti X.Pan Y.Pan A.Pathak 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.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 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 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.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 Tao Yang Y.Yang Y.F.Yang Y.X.Yang Yifan 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 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 Shuihan Zhang Shulei Zhang X.D.Zhang X.M.Zhang X.Y.Zhang Y.Zhang Y.T.Zhang Y.H.Zhang Y.M.Zhang Yan Zhang Yao 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 Lei Zhao Ling 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 J.Zhu K.Zhu K.J.Zhu K.S.Zhu L.Zhu L.X.Zhu S.H.Zhu S.Q.Zhu T.J.Zhu W.D.Zhu Y.C.Zhu Z.A.Zhu J.H.Zou J.Zu 《Chinese Physics C》 SCIE CAS CSCD 2024年第9期8-20,共13页
The number ofψ(3686)events collected by the BESⅢdetector during the 2021 run period is determined to be(2259.3±11.1)×10~6 by counting inclusiveψ(3686)hadronic events.The uncertainty is systematic and the ... The number ofψ(3686)events collected by the BESⅢdetector during the 2021 run period is determined to be(2259.3±11.1)×10~6 by counting inclusiveψ(3686)hadronic events.The uncertainty is systematic and the statistical uncertainty is negligible.Meanwhile,the numbers ofψ(3686)events collected during the 2009 and 2012run periods are updated to be(107.7±0.6)×10~6 and(345.4±2.6)×10~6,respectively.Both numbers are consistent with the previous measurements within one standard deviation.The total number ofψ(3686)events in the three data samples is(2712.4±14.3)×10~6. 展开更多
关键词 ψ(3686) inclusive process Hadronic events BESⅢdetector
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Optimization of performance of the KM2A full array using the Crab Nebula
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作者 曹臻 F.Aharonian +275 位作者 安琪 阿西克古 白云翔 包逸炜 D.Bastieri 毕效军 毕玉江 蔡金庭 曹晴 曹文羽 曹喆 常进 常劲帆 陈尚明 陈恩生 陈亮 陈林 陈龙 陈明君 陈玛丽 陈起辉 陈素弘 陈天禄 陈阳 程宁 程耀东 崔明阳 崔树旺 崔晓红 崔昱东 戴本忠 代洪亮 戴子高 单增罗布 D.della Volpe 董绪强 段凯凯 樊军辉 范一中 方军 方堃 冯存峰 封莉 冯少辉 丰晓婷 冯有亮 S.Gabici 高博 高川东 高林青 高启 高卫 高伟康 葛茂茂 耿利斯 G.Giacinti 龚光华 苟全补 顾旻皓 郭福来 郭晓磊 郭义庆 郭莹莹 韩毅昂 何会海 贺昊宁 何佳银 何新波何钰 M.Heller 贺远强 侯博文 侯超 侯贤 胡红波 胡铨 胡世聪 黄代绘 黄天奇 黄文俊 黄性涛 黄晓渊 黄勇 黄志成 季筱璐 贾焕玉 贾康 江琨 姜晓巍 姜泽军 金敏 康明铭 柯通 D.Kuleshov.K.Kurinov 李兵兵 李澄 李骢 李丹 李飞 李海波 李会财 李华阳 李军 李剑 李捷 李凯 李文龙 李文莲 李秀荣 李昕 李一卓 李哲 黎卓 梁恩维 梁云峰 林苏杰 刘冰 刘成 刘栋 刘虎 刘海东 刘佳 刘江来 刘金艳 刘茂元 柳若愚 刘四明 刘伟 刘怡 刘以农 鲁睿 罗晴 吕洪魁 马伯强 马玲玲 马欣华 毛基荣 闵振 W.Mitthumsiri 穆慧君 南云程 A.Neronov 区子维 庞彬宇 P.Pattarakijwanich 裴致远 齐孟尧 祁业情 乔冰强 秦家军 D.Ruffolo A.Sáiz D.Semikoz 邵澄宇 邵琅 O.Shchegolev 盛祥东 舒富文 宋慧超 Yu.V.Stenkin V.Stepanov 苏扬 孙秦宁 孙晓娜 孙志斌 谭柏轩 唐庆文 唐泽波 田文武 王超 王昌贝 王广威 王洪光 王惠惠 王建成 汪凯 王利苹 王玲玉 王培汉 王冉 王为 王祥高 王祥玉 王阳 王玉东 王岩谨 王忠海 王仲翔 王振 王铮 韦大明 魏俊杰 魏永健 文韬 吴超勇 吴含荣 武莎 吴雪峰 吴雨生 席邵强 夏捷 夏君集 项光漫 肖迪泫 肖刚 辛广广 辛玉良 邢祎 熊峥 徐东莲 徐仁峰 徐仁新 徐伟立 薛良 闫大海 颜景志 颜田 杨朝文 杨帆 杨冯帆 杨何文 杨佳盈 杨莉莉 杨明洁 杨睿智 杨深邦 姚玉华 姚志国 叶一锰 尹丽巧 尹娜 游晓浩 游智勇 于艳红 袁强 岳华 曾厚敦 曾婷轩 曾玮 查敏 张彬彬 张丰 张海明 张恒英 张建立 张丽霞 张力 张鹏飞 张佩佩 张瑞 张少博 张少如 张寿山 张潇 张笑鹏 张云峰 张毅 张勇 赵兵 赵静 赵雷 赵立志 赵世平 郑福 周斌 周浩 周佳能 周猛 周平 周荣 周勋秀 祝成光 祝凤荣 朱辉 朱科军 左雄 LHAASO Collaboration 《Chinese Physics C》 SCIE CAS CSCD 2024年第6期169-178,共10页
The full array of the Large High Altitude Air Shower Observatory(LHAASO)has been in operation since July 2021.For its kilometer-square array(KM2A),we optimized the selection criteria for very high and ultrahigh energy... The full array of the Large High Altitude Air Shower Observatory(LHAASO)has been in operation since July 2021.For its kilometer-square array(KM2A),we optimized the selection criteria for very high and ultrahigh energyγ-rays using data collected from August 2021 to August 2022,resulting in an improvement in significance of the detection in the Crab Nebula of approximately 15%,compared with that of previous cuts.With the implementation of these new selection criteria,the angular resolution was also significantly improved by approximately 10%at tens of TeV.Other aspects of the full KM2A array performance,such as the pointing error,were also calibrated using the Crab Nebula.The resulting energy spectrum of the Crab Nebula in the energy range of 10-1000 TeV are well fitted by a log-parabola model,which is consistent with the previous results from LHAASO and other experiments. 展开更多
关键词 Γ-RAY Crab Nebula SIGNIFICANCE
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Search for hidden-charm tetraquark with strangeness in e^(+)e^(−)→K^(+)D_(s)^(∗−) D^(∗0 )+ c.c.
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作者 麦迪娜 M.N.Achasov +579 位作者 P.Adlarson M.Albrecht R.Aliberti A.Amoroso 安美儒 安琪 白羽 O.Bakina R.Baldini Ferroli I.Balossino Y.Ban V.Batozskaya D.Becker K.Begzsuren N.Berger M.Bertani D.Bettoni F.Bianchi E.Bianco J.Bloms A.Bortone I.Boyko R.A.Briere A.Brueggemann 蔡浩 蔡啸 A.Calcaterra 曹国富 曹宁 S.A.Cetin 常劲帆 常万玲 车国荣 G.Chelkov 陈琛 陈超 陈刚 陈和生 陈玛丽 陈申见 陈少敏 T.Chen 陈旭荣 X.T.Chen 陈元柏 陈卓俊 成伟帅 S.K.Choi 初晓 G.Cibinetto F.Cossio 崔佳佳 代洪亮 代建平 A.Dbeyssi R.E.de Boer D.Dedovich 邓子艳 A.Denig I.Denysenko M.Destefanis F.De Mori 丁勇 丁逸 董静 董燎原 董明义 董翔 杜书先 段宗欢 P.Egorov 范玉兰 方建 房双世 方文兴 方易 R.Farinelli L.Fava F.Feldbauer G.Felici 封常青 冯俊华 K Fischer M.Fritsch C.Fritzsch 傅成栋 高涵 高原宁 高扬 S.Garbolino I.Garzia 葛潘婷 葛振武 耿聪 E.M.Gersabeck A Gilman K.Goetzen 龚丽 龚文煊 W.Gradl M.Greco 谷立民 顾旻皓 顾运厅 关春懿 郭爱强 郭立波 郭如盼 郭玉萍 A.Guskov 韩文颖 郝喜庆 F.A.Harris 何凯凯 何康林 F.H.Heinsius C.H.Heinz 衡月昆 C.Herold 侯国一 侯颖锐 侯治龙 胡海明 J.F.Hu 胡涛 胡誉 黄光顺 黄凯旋 黄麟钦 黄性涛 黄燕萍 黄震 T.Hussain N Hüsken W.Imoehl M.Irshad J.Jackson S.Jaeger S.Janchiv E.Jang J.H.Jeong 纪全 姬清平 季晓斌 季筱璐 吉钰瑶 贾泽坤 蒋沛成 姜赛赛 江晓山 Y.Jiang 焦健斌 焦铮 金山 金毅 荆茂强 T.Johansson S.Kabana N.Kalantar-Nayestanaki 康晓琳 康晓珅 R.Kappert M.Kavatsyuk 柯百谦 I.K.Keshk A.Khoukaz R.Kiuchi R.Kliemt L.Koch O.B.Kolcu B.Kopf M.Kuemmel M.Kuessner A.Kupsc W.Kühn J.J.Lane J.S.Lange P.Larin A.Lavania L.Lavezzi 雷天天 雷祚弘 H.Leithoff M.Lellmann T.Lenz 李聪 李翠 李春花 李澄 李德民 李飞 李刚 李慧 李贺 李海波 李惠静 H.N.Li J.Q.Li 李静舒 李井文 李科 L.J Li 李龙科 李蕾 李明浩 李培荣 李素娴 栗帅迎 李腾 李卫东 李卫国 李旭红 李晓玲 李晓宇 李彦谷 李振轩 李紫源 梁畅 梁浩 梁昊 梁勇飞 梁羽铁 廖广睿 廖龙洲 J.Libby A.Limphirat 林创新 林德旭 T.Lin 刘北江 刘成 刘春秀 D.Liu 刘福虎 刘芳 刘峰 G.M.Liu h.liu 刘宏邦 刘怀民 刘欢欢 刘汇慧 刘建北 刘佳俊 刘晶译 刘凯 刘魁勇 刘珂 刘亮 刘露 刘美宏 刘佩莲 刘倩 刘树彬 刘桐 刘维克 刘卫民 刘翔 刘英 刘玉斌 刘振安 刘智青 娄辛丑 卢飞翔 吕海江 吕军光 陆小玲 卢宇 卢云鹏 卢泽辉 罗成林 罗民兴 罗涛 罗小兰 吕晓睿 吕翌丰 马凤才 马海龙 马连良 马明明 马秋梅 马润秋 马瑞廷 马骁妍 马尧 F.E.Maas M.Maggiora S.Maldaner S.Malde Q.A.Malik A.Mangoni 冒亚军 毛泽普 S.Marcello 孟召霞 J.G.Messchendorp G.Mezzadri H.Miao 闵天觉 R.E.Mitchell 莫晓虎 N.Yu.Muchnoi Y.Nefedov F.Nerling I.B.Nikolaev 宁哲 S.Nisar 牛艳 S.L.Olsen 欧阳群 S.Pacetti 潘祥 潘越 A.Pathak 裴宇鹏 M.Pelizaeus 彭海平 K.Peters 平加伦 平荣刚 S.Plura S.Pogodin V.Prasad 齐法制 齐航 漆红荣 祁鸣 齐天钰 钱森 钱文斌 钱圳 乔从丰 秦佳佳 秦丽清 覃潇平 秦小帅 秦中华 邱进发 屈三强 K.H.Rashid C.F.Redmer 任旷洁 A.Rivetti V.Rodin M.Rolo 荣刚 Ch.Rosner 阮氏宁 A.Sarantsev Y.Schelhaas C.Schnier K.Schoenning M.Scodeggio 尚科羽 单葳 单心钰 上官剑锋 邵立港 邵明 沈成平 沈宏飞 沈文涵 沈肖雁 施伯安 石煌超 石京燕 石勤强 师荣盛 史欣 宋娇娇 宋维民 宋昀轩 S.Sosio S.Spataro F.Stieler 苏彭彭 粟杨捷 孙功星 H.Sun 孙浩凯 孙俊峰 孙亮 孙胜森 孙童 孙文玉 孙勇杰 孙永昭 孙振田 谭英华 谭雅星 唐昌建 唐光毅 唐健 陶璐燕 陶秋田 M.Tat 滕佳秀 V.Thoren 田文辉 田野 I.Uman 王斌 王博 王滨龙 王成伟 王大勇 王菲 王泓鉴 王宏鹏 王科 王亮亮 王萌 王梦真 王蒙 王顺 S.Wang 王婷 王腾蛟 王为 王文欢 王维平 王轩 王雄飞 王小龙 王亦 王雅迪 王贻芳 王英豪 王雨晴 王亚乾 王铮 王至勇 王子一 魏代会 F.Weidner 文硕频 D.J.White U.Wiedner G.Wilkinson M.Wolke L.Wollenberg 吴金飞 伍灵慧 吴连近 吴潇 伍雄浩 Y.Wu 吴英杰 吴智 夏磊 相腾 肖栋 肖光延 肖浩 肖素玉 肖云龙 肖振军 谢陈 谢昕海 谢勇 谢宇广 谢跃红 谢智鹏 邢天宇 C.F.Xu 许创杰 许国发 许皓月 徐庆君 徐新平 胥英超 许泽鹏 严芳 严亮 鄢文标 闫文成 杨海军 杨昊霖 杨洪勋 杨涛 杨艳芳 杨逸翔 杨翊凡 叶梅 叶铭汉 殷俊昊 尤郑昀 俞伯祥 喻纯旭 余刚 于涛 余旭东 苑长征 袁丽 S.C.Yuan 袁晓庆 袁野 袁朝阳 岳崇兴 A.A.Zafar 曾凡蕊 曾鑫 曾云 翟星晔 詹永华 张安庆 B.L.Zhang 张丙新 张丹昊 张广义 H.Zhang 张宏宏 张宏浩 张华桥 章红宇 张杰磊 张敬庆 张家文 J.X.Zhang 张建勇 张景芝 张剑宇 张嘉伟 张黎明 L.Q.Zhang 张雷 P.Zhang 张秋岩 张水涵 张书磊 张小东 X.M.Zhang 张学尧 张旭颜 Y.Zhang 张亚腾 张银鸿 张言 张瑶 Z.H.Zhang 张兆领 张子羽 张振宇 赵光 赵静 赵静宜 赵京周 赵雷 赵玲 赵明刚 赵书俊 赵豫斌 赵宇翔 赵政国 A.Zhemchugov 郑波 郑建平 郑阳恒 钟彬 钟翠 钟鑫 周航 周利鹏 周详 周晓康 周小蓉 周兴玉 周袆卓 朱江 朱凯 朱科军 朱琳萱 朱世海 朱仕强 朱腾蛟 朱文静 朱莹春 朱自安 邹佳恒 祖健 《Chinese Physics C》 SCIE CAS CSCD 2023年第3期1-14,共14页
We report a search for a heavier partner of the recently observed Z_(cs)(3985)^(-) state,denoted as Z_(cs)^('-),in the process e^(+)e^(−)→K^(+)D_(s)^(∗−) D^(∗0 )+ c.c.,based on e^(*)e^(-)collision data collected ... We report a search for a heavier partner of the recently observed Z_(cs)(3985)^(-) state,denoted as Z_(cs)^('-),in the process e^(+)e^(−)→K^(+)D_(s)^(∗−) D^(∗0 )+ c.c.,based on e^(*)e^(-)collision data collected at the center-of-mass energies of √s=4.661,4.682 and 4.699 GeV with the BESIII detector.The Z_(cs)^('-) is of interest as it is expected to be a candidate for a hidden-charm and open-strange tetraquark.A partial-reconstruction technique is used to isolate K^(+)recoil-mass spectra,which are probed for a potential contribution from Z_(cs)^('-)→D_(s)^(∗−) D^(∗0 )+ c.c.We find an excess of Z_(cs)^('-)→D_(s)^(*-)-D^(*0)(c.c.)candidates with a significance of 2.1o,after considering systematic uncertainties,at a mass of(4123.5±0.7_(sat)±4.7_(syst.))MeV/c^(2).As the data set is limited in size,the upper limits are evaluated at the 90%confidence level on the product of the Born cross sections(σ^(Borm))and the branching fraction(B)of Z_(cs)^('-)→D_(s)^(*-)-D^(*0),under different assumptions of the Z_(cs)^('-) mass from 4.120 to 4.140 MeV and of the width from 10 to 50 MeV at the three center-of-mass energies.The upper limits of σ^(Born).B are found to be at the level of O(1)pb at each energy.Larger data samples are needed to confirm the Z_(cs)^('-) state and clarify its nature in the coming years. 展开更多
关键词 electron-positron collision BESIl hadron spectroscopy TETRAQUARK
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Search for the weak decayψ(3686)→■+c.c.
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作者 麦迪娜 M.N.Achasov +568 位作者 P.Adlarson M.Albrecht R.Aliberti A.Amoroso 安美儒 安琪 白旭红 白羽 O.Bakina R.Baldini Ferroli I.Balossino 班勇 V.Batozskaya D.Becker K.Begzsuren N.Berger M.Bertani D.Bettoni F.Bianchi J.Bloms A.Bortone I.Boyko R.A.Briere A.Brueggemann 蔡浩 蔡啸 A.Calcaterra 曹国富 曹宁 S.A.Cetin 常劲帆 常万玲 G.Chelkov 陈琛 陈超 陈刚 陈和生 陈玛丽 陈申见 陈少敏 T.Chen 陈旭荣 X.T.Chen 陈元柏 陈卓俊 成伟帅 初晓 G.Cibinetto F.Cossio 崔佳佳 代洪亮 代建平 A.Dbeyssi R.E.de Boer D.Dedovich 邓子艳 A.Denig I.Denysenko M.Destefanis F.De Mori 丁勇 董静 董燎原 董明义 董翔 杜书先 P.Egorov 范玉兰 方建 房双世 方文兴 方易 R.Farinelli L.Fava F.Feldbauer G.Felici 封常青 冯俊华 K Fischer M.Fritsch C.Fritzsch 傅成栋 高涵 高原宁 高扬 S.Garbolino I.Garzia 葛潘婷 葛振武 耿聪 E.M.Gersabeck A Gilman K.Goetzen 龚丽 龚文煊 W.Gradl M.Greco 谷立民 顾旻皓 顾运厅 关春懿 郭爱强 郭立波 郭如盼 郭玉萍 A.Guskov 韩婷婷 韩文颖 郝喜庆 F.A.Harris 何凯凯 何康林 F.H.Heinsius C.H.Heinz 衡月昆 C.Herold M.Himmelreich 侯国一 侯颖锐 侯治龙 胡海明 J.F.Hu 胡涛 胡誉 黄光顺 黄凯旋 黄麟钦 黄麟钦 黄性涛 黄燕萍 黄震 T.Hussain N Hüsken W.Imoehl M.Irshad J.Jackson S.Jaeger S.Janchiv 纪全 姬清平 季晓斌 季筱璐 吉钰瑶 贾泽坤 姜侯兵 姜赛赛 江晓山 Y.Jiang 焦健斌 焦铮 金山 金毅 荆茂强 T.Johansson N.Kalantar-Nayestanaki 康晓珅 R.Kappert 柯百谦 I.K.Keshk A.Khoukaz P.Kiese R.Kiuchi R.Kliemt L.Koch O.B.Kolcu B.Kopf M.Kuemmel M.Kuessner A.Kupsc W.Kühn J.J.Lane J.S.Lange P.Larin A.Lavania L.Lavezzi 雷祚弘 H.Leithoff M.Lellmann T.Lenz 李翠 李聪 李春花 李澄 李德民 李飞 李刚 李慧 李贺 李海波 李惠静 H.N.Li J.Q.Li 李静舒 李井文 李科 L.J.Li 李龙科 李蕾 李明浩 李培荣 李素娴 栗帅迎 李腾 李卫东 李卫国 李旭红 李晓玲 李晓宇 梁昊 梁浩 梁浩 梁勇飞 梁羽铁 廖广睿 廖龙洲 J.Libby A.Limphirat 林创新 林德旭 T.Lin 刘北江 刘春秀 D.Liu 刘福虎 刘芳 刘峰 G.M.Liu h.liu 刘宏邦 刘怀民 刘欢欢 刘汇慧 刘建北 刘佳俊 刘晶译 刘凯 刘魁勇 刘珂 刘亮 刘露 刘美宏 刘佩莲 刘倩 刘树彬 刘桐 刘维克 刘卫民 刘翔 刘英 刘玉斌 刘振安 刘智青 娄辛丑 卢飞翔 吕海江 吕军光 陆小玲 卢宇 卢云鹏 Z.H.Lu 罗成林 罗民兴 罗涛 罗小兰 吕晓睿 吕翌丰 马凤才 马海龙 马连良 马明明 马秋梅 马润秋 马瑞廷 马骁妍 马尧 F.E.Maas M.Maggiora S.Maldaner S.Malde Q.A.Malik A.Mangoni 冒亚军 毛泽普 S.Marcello 孟召霞 J.G.Messchendorp G.Mezzadri H.Miao 闵天觉 R.E.Mitchell 莫晓虎 N.Yu.Muchnoi Y.Nefedov F.Nerling I.B.Nikolaev 宁哲 S.Nisar 牛艳 S.L.Olsen 欧阳群 S.Pacetti 潘祥 潘越 A.Pathak M.Pelizaeus 彭海平 K.Peters 平加伦 平荣刚 S.Plura S.Pogodin V.Prasad 齐法制 齐航 漆红荣 祁鸣 齐天钰 钱森 钱文斌 钱圳 乔从丰 秦佳佳 秦丽清 覃潇平 秦小帅 秦中华 邱进发 屈三强 K.H.Rashid C.F.Redmer 任旷洁 A.Rivetti V.Rodin M.Rolo 荣刚 Ch.Rosner 阮氏宁 桑昊榆 A.Sarantsev Y.Schelhaas C.Schnier K.Schoenning M.Scodeggio 尚科羽 单葳 单心钰 上官剑锋 邵立港 邵明 沈成平 沈宏飞 沈肖雁 施伯安 石煌超 石京燕 石勤强 师荣盛 史欣 师晓东 宋娇娇 宋维民 宋昀轩 S.Sosio S.Spataro F.Stieler 苏可馨 苏彭彭 粟杨捷 孙功星 H.Sun 孙浩凯 孙俊峰 孙亮 孙胜森 孙童 孙文玉 孙翔 孙勇杰 孙永昭 孙振田 谭英华 谭雅星 唐昌建 唐光毅 唐健 陶璐燕 陶秋田 M.Tat 滕佳秀 V.Thoren 田文辉 田野 I.Uman 王斌 王滨龙 王成伟 王大勇 王菲 王泓鉴 王宏鹏 王科 王亮亮 王萌 王梦真 王蒙 S.Wang 王顺 王婷 王腾蛟 王为 王文欢 王维平 王轩 王雄飞 王小龙 王亦 王雅迪 王贻芳 王英豪 王雨晴 王亚乾 王铮 王至勇 王子一 魏代会 F.Weidner 文硕频 D.J.White U.Wiedner G.Wilkinson M.Wolke L.Wollenberg 吴金飞 伍灵慧 吴连近 吴潇 伍雄浩 Y.Wu 吴智 夏磊 相腾 肖栋 肖光延 肖浩 肖素玉 肖云龙 肖振军 谢陈 谢昕海 谢勇 谢宇广 谢跃红 谢智鹏 邢天宇 C.F.Xu 许创杰 许国发 许皓月 徐庆君 徐新平 胥英超 许泽鹏 严芳 严亮 鄢文标 闫文成 杨海军 杨昊霖 杨洪勋 杨玲 杨双莉 杨涛 杨艳芳 杨逸翔 杨翊凡 叶梅 叶铭汉 殷俊昊 尤郑昀 俞伯祥 喻纯旭 余刚 于涛 苑长征 袁丽 S.C.Yuan 袁晓庆 袁野 袁朝阳 岳崇兴 A.A.Zafar 曾凡蕊 曾鑫 曾云 詹永华 张安庆 B.L.Zhang 张丙新 张丹昊 张广义 H.Zhang 张宏浩 张宏宏 章红宇 张杰磊 张敬庆 张家文 J.X.Zhang 张建勇 张景芝 张剑宇 张嘉伟 张黎明 张丽青 张雷 P.Zhang 张秋岩 张水涵 张书磊 张小东 X.M.Zhang 张学尧 张旭颜 Y.Zhang 张亚腾 张银鸿 张言 张瑶 Z.H.Zhang 张振宇 张子羽 赵光 赵静 赵静宜 赵京周 赵雷 赵玲 赵明刚 赵强 赵书俊 赵豫斌 赵宇翔 赵政国 A.Zhemchugov 郑波 郑建平 郑阳恒 钟彬 钟翠 钟鑫 周航 周利鹏 周详 周晓康 周小蓉 周兴玉 周袆卓 朱江 朱凯 朱科军 朱琳萱 朱世海 朱仕强 朱腾蛟 朱文静 朱莹春 朱自安 邹冰松 邹佳恒 《Chinese Physics C》 SCIE CAS CSCD 2023年第1期19-27,共9页
Using(448.1±2.9)×10^(6)ψ(3686)for the weak baryonic decayψ(3686)→Λc+∑-+c.c..The analysis procedure is optimized using a blinded method.No significant signal is observed,and the upper limit on the branch... Using(448.1±2.9)×10^(6)ψ(3686)for the weak baryonic decayψ(3686)→Λc+∑-+c.c..The analysis procedure is optimized using a blinded method.No significant signal is observed,and the upper limit on the branching fraction(B)ofψ(3686)→Λc+∑-+c.c.is set as 1.4×10^(-5)at the 90%confidence level. 展开更多
关键词 weak decay upper limit BESIII detector
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Observations of the Cabibbo-Suppressed decays Λ_(c)^(+)→nπ+π^(0),nπ^(+)π^(-)π^(+) and the Cabibbo-Favored decay Λ_(c)^(+)→nK^(-)π^(+)π^(+)
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作者 麦迪娜 M.N.Achasov +576 位作者 P.Adlarson M.Albrecht R.Aliberti A.Amoroso 安美儒 安琪 白羽 O.Bakina R.Baldini Ferroli I.Balossino 班勇 V.Batozskaya D.Becker K.Begzsuren N.Berger M.Bertani D.Bettoni F.Bianchi E.Bianco J.Bloms A.Bortone I.Boyko R.A.Briere A.Brueggemann 蔡浩 蔡啸 A.Calcaterra 曹国富 曹宁 S.A.Cetin 常劲帆 常万玲 车国荣 G.Chelkov 陈琛 陈超 陈刚 陈和生 陈玛丽 陈申见 陈少敏 T.Chen 陈旭荣 X.T.Chen 陈元柏 陈卓俊 成伟帅 S.K.Choi 初晓 G.Cibinetto F.Cossio 崔佳佳 代洪亮 代建平 A.Dbeyssi R.Ede Boer D.Dedovich 邓子艳 A.Denig I.Denysenko M.Destefanis F.De Mori 丁勇 丁逸 董静 董燎原 董明义 董翔 杜书先 段宗欢 P.Egorov 范玉兰 方建 房双世 方文兴 方易 R.Farinelli L.Fava F.Feldbauer G.Felici 封常青 冯俊华 K Fischer M.Fritsch C.Fritzsch 傅成栋 高涵 高原宁 高扬 S.Garbolino I.Garzia 葛潘婷 葛振武 耿聪 E.M.Gersabeck A Gilman K.Goetzen 龚丽 龚文煊 W.Gradl M.Greco 谷立民 顾旻皓 顾运厅 关春懿 郭爱强 郭立波 郭如盼 郭玉萍 A.Guskov 韩文颖 郝喜庆 F.A.Harris 何凯凯 何康林 F.H.Heinsius C.H.Heinz 衡月昆 C.Herold 侯国一 侯颖锐 侯治龙 胡海明 J.F.Hu 胡涛 胡誉 黄光顺 黄凯旋 黄麟钦 黄性涛 黄燕萍 黄震 T.Hussain N Hüsken W.Imoehl M.Irshad J.Jackson S.Jaeger S.Janchiv E.Jang J.H.Jeong 纪全 姬清平 季晓斌 季筱璐 吉钰瑶 贾泽坤 姜赛赛 江晓山 Y.Jiang 焦健斌 焦铮 金山 金毅 荆茂强 T.Johansson N.Kalantar-Nayestanaki 康晓珅 R.Kappert M.Kavatsyuk 柯百谦 I.K.Keshk A.Khoukaz R.Kiuchi R.Kliemt L.Koch O.B.Kolcu B.Kopf M.Kuemmel M.Kuessner A.Kupsc W.Kühn J.J.Lane J.S.Lange P.Larin A.Lavania L.Lavezzi 雷祚弘 H.Leithoff M.Lellmann T.Lenz 李翠 李聪 李春花 李澄 李德民 李飞 李刚 李慧 李贺 李海波 李惠静 H.N.Li J.Q.Li 李静舒 李井文 李科 L.J Li 李龙科 李蕾 李明浩 李培荣 李素娴 栗帅迎 李腾 李卫东 李卫国 李旭红 李晓玲 李晓宇 李彦谷 李振轩 李紫源 梁畅 梁昊 梁浩 梁浩 梁勇飞 梁羽铁 廖广睿 廖龙洲 J.Libby A.Limphirat 林创新 林德旭 T.Lin 刘北江 刘成 刘春秀 D.Liu 刘福虎 刘芳 刘峰 G.M.Liu h.liu 刘宏邦 刘怀民 刘欢欢 刘汇慧 刘建北 刘佳俊 刘晶译 刘凯 刘魁勇 刘珂 刘亮 刘露 刘美宏 刘佩莲 刘倩 刘树彬 刘桐 刘维克 刘卫民 刘翔 刘英 刘玉斌 刘振安 刘智青 娄辛丑 卢飞翔 吕海江 吕军光 陆小玲 卢宇 卢云鹏 Z.H.Lu 罗成林 罗民兴 罗涛 罗小兰 吕晓睿 吕翌丰 马凤才 马海龙 马连良 马明明 马秋梅 马润秋 马瑞廷 马骁妍 马尧 F.E.Maas M.Maggiora S.Maldaner S.Malde Q.A.Malik A.Mangoni 冒亚军 毛泽普 S.Marcello 孟召霞 J.G.Messchendorp G.Mezzadri H.Miao 闵天觉 R.E.Mitchell 莫晓虎 N.Yu.Muchnoi Y.Nefedov F.Nerling I.B.Nikolaev 宁哲 S.Nisar 牛艳 S.L.Olsen 欧阳群 S.Pacetti 潘祥 潘越 A.Pathak P.Patteri M.Pelizaeus 彭海平 K.Peters 平加伦 平荣刚 S.Plura S.Pogodin V.Prasad 齐法制 齐航 漆红荣 祁鸣 齐天钰 钱森 钱文斌 钱圳 乔从丰 秦佳佳 秦丽清 覃潇平 秦小帅 秦中华 邱进发 屈三强 K.H.Rashid C.F.Redmer 任旷洁 A.Rivetti V.Rodin M.Rolo 荣刚 Ch.Rosner 阮氏宁 A.Sarantsev Y.Schelhaas C.Schnier K.Schoenning M.Scodeggio 尚科羽 单葳 单心钰 上官剑锋 邵立港 邵明 沈成平 沈宏飞 沈肖雁 施伯安 石煌超 石京燕 石勤强 师荣盛 史欣 师晓东 宋娇娇 宋维民 宋昀轩 S.Sosio S.Spataro F.Stieler 苏可馨 苏彭彭 粟杨捷 孙功星 HSun 孙浩凯 孙俊峰 孙亮 孙胜森 孙童 孙文玉 孙勇杰 孙永昭 孙振田 谭英华 谭雅星 唐昌建 唐光毅 唐健 陶璐燕 陶秋田 M.Tat 滕佳秀 V.Thoren 田文辉 田野 I.Uman 王斌 王滨龙 王成伟 王大勇 王菲 王泓鉴 王宏鹏 王科 王亮亮 王萌 王梦真 王蒙 S.Wang 王顺 王婷 王腾蛟 王为 王文欢 王维平 王轩 王雄飞 王小龙 王亦 王雅迪 王贻芳 王英豪 王雨晴 王亚乾 王铮 王至勇 王子一 魏代会 F.Weidner 文硕频 D.J.White U.Wiedner G.Wilkinson M.Wolke L.Wollenberg 吴金飞 伍灵慧 吴连近 吴潇 伍雄浩 Y.Wu 吴英杰 吴智 夏磊 相腾 肖栋 肖光延 肖浩 肖素玉 肖云龙 肖振军 谢陈 谢昕海 谢勇 谢宇广 谢跃红 谢智鹏 邢天宇 C.F.Xu 许创杰 许国发 许皓月 徐庆君 徐新平 胥英超 许泽鹏 严芳 严亮 鄢文标 闫文成 杨海军 杨昊霖 杨洪勋 杨玲 杨涛 杨艳芳 杨逸翔 杨翊凡 叶梅 叶铭汉 殷俊昊 尤郑昀 俞伯祥 喻纯旭 余刚 于涛 余旭东 苑长征 袁丽 S.C.Yuan 袁晓庆 袁野 袁朝阳 岳崇兴 A.A.Zafar 曾凡蕊 曾鑫 曾云 翟星晔 詹永华 张安庆 B.L.Zhang 张丙新 张丹昊 张广义 H.Zhang 张宏浩 张宏宏 章红宇 张杰磊 张敬庆 张家文 J.X.Zhang 张建勇 张景芝 张剑宇 张嘉伟 张黎明 张丽青 张雷 P.Zhang 张秋岩 张水涵 张书磊 张小东 X.M.Zhang 张学尧 张旭颜 Y.Zhang 张亚腾 张银鸿 张言 张瑶 Z.H.Zhang 张兆领 张振宇 张子羽 赵光 赵静 赵静宜 赵京周 赵雷 赵玲 赵明刚 赵书俊 赵豫斌 赵宇翔 赵政国 A.Zhemchugov 郑波 郑建平 郑阳恒 钟彬 钟翠 钟鑫 周航 周利鹏 周详 周晓康 周小蓉 周兴玉 周袆卓 朱江 朱凯 朱科军 朱琳萱 朱世海 朱仕强 朱腾蛟 朱文静 朱莹春 朱自安 邹佳恒 M.Ablikim 《Chinese Physics C》 SCIE CAS CSCD 2023年第2期1-18,共18页
Using electron-positron annihilation data samples corresponding to an integrated luminosity of 4.5 fb-1,collected by the BESⅢdetector in the energy region between 4599.53 MeV and 4698.82 MeV,we report the first obser... Using electron-positron annihilation data samples corresponding to an integrated luminosity of 4.5 fb-1,collected by the BESⅢdetector in the energy region between 4599.53 MeV and 4698.82 MeV,we report the first observations of the Cabibbo-suppressed decaysΛ_(c)^(+)→nπ^(+)π^(0),Λ_(c)^(+)→nπ^(+)π^(-)π^(+),and the Cabibbo-favored decayΛ_(c)^(+)→nK^(-)π^(+)π^(+)with statistical significances of 7.9σ,7.8σ,and>10σ,respectively.The branching fractions of these decays are measured to be B(Λ_(c)^(+)→nπ^(+)π^(0))=(0.64±0.09±0.02)%,B(Λ_(c)^(+)→nπ^(+)π^(-)π^(+))=(0.45±0.07±0.03)%,and B(Λ_(c)^(+)→nK^(-)π^(+)π^(+))=(1.90±0.08±0.09)%,where the first uncertainties are statistical and the second are systematic.We find that the branching fraction of the decayΛ_(c)^(+)→nπ^(+)π^(0)is about one order of magnitude higher than that ofΛ_(c)^(+)→nπ^(+). 展开更多
关键词 ∧_(c)^(+)baryon Branching fraction BESⅢdetector
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Flux variations of cosmic ray air showers detected by LHAASO-KM2A during a thunderstorm on June 10,2021
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作者 F.Aharonian 安琪 +270 位作者 阿西克古 白立新 白云翔 包逸炜 D.Bastieri 毕效军 毕玉江 蔡金庭 曹喆 曹臻 常进 常劲帆 陈恩生 陈良 陈亮 陈龙 陈明君 陈玛丽 陈素弘 陈松战 陈天禄 陈学健 陈阳 程皓麟 程宁 程耀东 崔树旺 崔晓红 崔昱东 戴本忠 代洪亮 戴子高 单增罗布 D.della Volpe 段凯凯 樊军辉 范一中 范志香 方军 方堃 冯存峰 封莉 冯少辉 丰晓婷 冯有亮 高博 高川东 高林青 高启 高卫 高伟康 葛茂茂 耿利斯 龚光华 苟全补 顾旻皓 郭福来 郭俊广 郭晓磊 郭义庆 郭莹莹 韩毅昂 何会海 贺昊宁 何思乐 何新波 何钰 M.Heller 贺远强 侯超 侯贤 胡红波 胡铨 胡森 胡世聪 呼晓军 黄代绘 黄文昊 黄性涛 黄晓渊 黄勇 黄志成 季筱璐 贾焕玉 贾康 江琨 姜泽军 金敏 康明铭 柯通 D.Kuleshov 李兵兵 李澄 李骢 李飞 李海波 李会财 李华阳 李军 李剑 李捷 李凯 李文龙 李秀荣 李昕 李新 李一卓 李哲 黎卓 梁恩维 梁云峰 林苏杰 刘冰 刘成 刘栋 刘虎 刘海东 刘佳 刘江来 刘佳松 刘金艳 刘茂元 柳若愚 刘四明 刘伟 刘怡 刘以农 龙文杰 鲁睿 罗晴 吕洪魁 马伯强 马玲玲 马欣华 毛基荣 A.Masood 闵振 W.Mitthumsiri 南云程 区子维 庞彬宇 P.Pattarakijwanich 裴致远 齐孟尧 祁业情 乔冰强 秦家军 D.Ruffolo A.Sáiz 邵澄宇 邵琅 O.Shchegolev 盛祥东 石京燕 宋慧超 Yu.V.Stenkin V.Stepanov 苏扬 孙秦宁 孙晓娜 孙志斌 谭柏轩 唐泽波 田文武 王博东 王超 王辉 王洪光 王建成 王界双 王利苹 王玲玉 王冉 王润娜 王为 王祥高 王祥玉 王阳 王玉东 王岩谨 王亚平 王忠海 王仲翔 王振 王铮 韦大明 魏俊杰 魏永健 文韬 吴超勇 吴含荣 武莎 吴雪峰 吴雨生 席邵强 夏捷 夏君集 项光漫 肖迪泫 肖刚 辛广广 辛玉良 邢祎 熊峥 徐东莲 徐仁新 薛良 闫大海 颜景志 杨朝文 杨冯帆 杨何文 杨佳盈 杨莉莉 杨明洁 杨睿智 杨深邦 姚玉华 姚志国 叶一锰 尹丽巧 尹娜 游晓浩 游智勇 于艳红 袁强 岳华 曾厚敦 曾婷轩 曾玮 曾宗康 查敏 翟徐徐 张彬彬 张丰 张海明 张恒英 张建立 张丽霞 张力 张路 张鹏飞 张佩佩 张瑞 张少博 张少如 张寿山 张潇 张笑鹏 张云峰 张月雷 张毅 张勇 赵兵 赵静 赵雷 赵立志 赵世平 郑福 郑应 周斌 周浩 周佳能 周平 周荣 周勋秀 祝成光 祝凤荣 朱辉 朱科军 左雄 《Chinese Physics C》 SCIE CAS CSCD 2023年第1期193-203,共11页
The Large High Altitude Air Shower Observatory(LHAASO)has three sub-arrays,KM2A,WCDA,and WFCTA.The flux variations of cosmic ray air showers were studied by analyzing the KM2A data during a thunderstorm on June 10,202... The Large High Altitude Air Shower Observatory(LHAASO)has three sub-arrays,KM2A,WCDA,and WFCTA.The flux variations of cosmic ray air showers were studied by analyzing the KM2A data during a thunderstorm on June 10,2021.The number of shower events that meet the trigger conditions increases significantly in atmospheric electric fields,with a maximum fractional increase of 20%.The variations in trigger rates(increases or decreases)were found to be strongly dependent on the primary zenith angle.The flux of secondary particles increased significantly,following a trend similar to that of shower events.To better understand the observed behavior,Monte Carlo simulations were performed with CORSIKA and G4KM2A(a code based on GEANT4).We found that the experimental data(in saturated negative fields)were in good agreement with the simulations,assuming the presence of a uniform electric field of-700 V/cm with a thickness of 1500 m in the atmosphere above the observation level.Due to the acceleration/deceleration by the atmospheric electric field,the number of secondary particles with energy above the detector threshold was modified,resulting in the changes in shower detection rate. 展开更多
关键词 THUNDERSTORM cosmic rays extensive air showers LHAASO-KM2A
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Search for the doubly heavy baryon Ξ_(bc)^(+)→ decaying to J/ψΞ_(c)^(+)
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作者 R.Aaij A.S.W.Abdelmotteleb +1013 位作者 C.Abellan Beteta F.Abudinén T.Ackernley B.Adeva M.Adinolfi H.Afsharnia C.Agapopoulou C.A.Aidala S.Aiola Z.Ajaltouni S.Akar K.Akiba J.Albrecht F.Alessio M.Alexander A.Alfonso Albero Z.Aliouche P.Alvarez Cartelle S.Amato J.L.Amey Y.Amhis L.An L.Anderlini M.Andersson A.Andreianov M.Andreotti D.Andreou D.Ao F.Archilli A.Artamonov M.Artuso E.Aslanides M.Atzeni B.Audurier S.Bachmann M.Bachmayer J.J.Back A.Bailly-reyre P.Baladron Rodriguez V.Balagura W.Baldini J.Baptista de Souza Leite M.Barbetti R.J.Barlow S.Barsuk W.Barter M.Bartolini F.Baryshnikov J.M.Basels G.Bassi B.Batsukh A.Battig A.Bay A.Beck M.Becker F.Bedeschi I.B.Bediaga A.Beiter V.Belavin S.Belin V.Bellee K.Belous I.Belov I.Belyaev G.Bencivenni E.Ben-Haim A.Berezhnoy R.Bernet D.Berninghoff H.C.Bernstein C.Bertella A.Bertolin C.Betancourt F.Betti Ia.Bezshyiko S.Bhasin J.Bhom L.Bian M.S.Bieker N.V.Biesuz S.Bifani P.Billoir A.Biolchini M.Birch F.C.R.Bishop A.Bitadze A.Bizzeti M.P.Blago T.Blake F.Blanc S.Blusk D.Bobulska J.A.Boelhauve O.Boente Garcia T.Boettcher A.Boldyrev N.Bondar S.Borghi M.Borsato J.T.Borsuk S.A.Bouchiba T.J.V.Bowcock A.Boyer C.Bozzi M.J.Bradley S.Braun A.Brea Rodriguez J.Brodzicka A.Brossa Gonzalo D.Brundu A.Buonaura L.Buonincontri A.T.Burke C.Burr A.Bursche A.Butkevich J.S.Butter J.Buytaert W.Byczynski S.Cadeddu H.Cai R.Calabrese L.Calefice S.Cali R.Calladine M.Calvi M.Calvo Gomez P.Camargo Magalhaes P.Campana D.H.Campora Perez A.F.Campoverde Quezada S.Capelli L.Capriotti A.Carbone G.Carboni R.Cardinale A.Cardini I.Carli P.Carniti L.Carus A.Casais Vidal R.Caspary G.Casse M.Cattaneo G.Cavallero V.Cavallini S.Celani J.Cerasoli D.Cervenkov A.J.Chadwick M.G.Chapman M.Charles Ph.Charpentier C.A.Chavez Barajas M.Chefdeville C.Chen S.Chen A.Chernov S.Chernyshenko V.Chobanova S.Cholak M.Chrzaszcz A.Chubykin V.Chulikov P.Ciambrone M.F.Cicala X.Cid Vidal G.Ciezarek G.Ciullo P.E.L.Clarke M.Clemencic H.V.Cliff J.Closier J.L.Cobbledick V.Coco J.A.B.Coelho J.Cogan E.Cogneras L.Cojocariu P.Collins T.Colombo L.Congedo A.Contu N.Cooke G.Coombs I.Corredoira G.Corti B.Couturier D.C.Craik J.Crkovská M.Cruz Torres R.Currie C.L.Da Silva S.Dadabaev L.Dai E.Dall'Occo J.Dalseno C.D'Ambrosio A.Danilina P.d'Argent J.E.Davies A.Davis O.De Aguiar Francisco J.de Boer K.De Bruyn S.De Capua M.De Cian U.De Freitas Carneiro Da Graca E.De Lucia J.M.De Miranda L.De Paula M.De Serio D.De Simone P.De Simone F.De Vellis J.A.de Vries C.T.Dean F.Debernardis D.Decamp V.Dedu L.Del Buono B.Delaney H.-P.Dembinski V.Denysenko O.Deschamps F.Dettori B.Dey A.Di Cicco P.Di Nezza S.Didenko L.Dieste Maronas S.Ding V.Dobishuk A.Dolmatov C.Dong A.M.Donohoe F.Dordei A.C.dos Reis L.Douglas A.G.Downes M.W.Dudek L.Dufour V.Duk P.Durante J.M.Durham D.Dutta A.Dziurda A.Dzyuba S.Easo U.Egede V.Egorychev S.Eidelman S.Eisenhardt S.Ek-In L.Eklund S.Ely A.Ene E.Epple S.Escher J.Eschle S.Esen T.Evans L.N.Falcao Y.Fan B.Fang S.Farry D.Fazzini M.Feo A.D.Fernez F.Ferrari L.Ferreira Lopes F.Ferreira Rodrigues S.Ferreres Sole M.Ferrillo M.Ferro-Luzzi S.Filippov R.A.Fini M.Fiorini M.Firlej K.M.Fischer D.S.Fitzgerald C.Fitzpatrick T.Fiutowski F.Fleuret M.Fontana F.Fontanelli R.Forty D.Foulds-Holt V.Franco Lima M.Franco Sevilla M.Frank E.Franzoso G.Frau C.Frei D.A.Friday J.Fu Q.Fuehring E.Gabriel G.Galati A.Gallas Torreira D.Galli S.Gambetta Y.Gan M.Gandelman P.Gandini Y.Gao M.Garau L.M.Garcia Martin P.Garcia Moreno J.García Pardiäas B.Garcia Plana F.A.Garcia Rosales L.Garrido C.Gaspar R.E.Geertsema D.Gerick L.L.Gerken E.Gersabeck M.Gersabeck T.Gershon L.Giambastiani V.Gibson H.K.Giemza A.L.Gilman M.Giovannetti A.Gioventù P.Gironella Gironell C.Giugliano M.A.Giza K.Gizdov E.L.Gkougkousis V.V.Gligorov C.Gäbel E.Golobardes D.Golubkov A.Golutvin A.Gomes S.Gomez Fernandez F.Goncalves Abrantes M.Goncerz G.Gong I.V.Gorelov C.Gotti J.P.Grabowski T.Grammatico L.A.Granado Cardoso E.Graugés E.Graverini G.Graziani A.T.Grecu L.M.Greeven N.A.Grieser L.Grillo S.Gromov B.R.Gruberg Cazon C.Gu 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M.Vesterinen D.Vieira M.Vieites Diaz X.Vilasis-Cardona E.Vilella Figueras A.Villa P.Vincent F.C.Volle D.vom Bruch A.Vorobyev V.Vorobyev N.Voropaev K.Vos R.Waldi J.Walsh C.Wang J.Wang J.Wang J.Wang J.Wang M.Wang R.Wang Y.Wang Z.Wang Z.Wang Z.Wang J.A.Ward N.K.Watson D.Websdale C.Weisser B.D.C.Westhenry D.J.White M.Whitehead A.R.Wiederhold D.Wiedner G.Wilkinson M.K.Wilkinson I.Williams M.Williams M.R.J.Williams R.Williams F.F.Wilson W.Wislicki M.Witek L.Witola C.P.Wong G.Wormser S.A.Wotton H.Wu K.Wyllie Z.Xiang D.Xiao Y.Xie A.Xu J.Xu L.Xu M.Xu Q.Xu Z.Xu Z.Xu D.Yang S.Yang Y.Yang Z.Yang Z.Yang L.E.Yeomans H.Yin J.Yu X.Yuan E.Zaffaroni M.Zavertyaev M.Zdybal O.Zenaiev M.Zeng D.Zhang L.Zhang S.Zhang S.Zhang Y.Zhang Y.Zhang A.Zharkova A.Zhelezov Y.Zheng T.Zhou X.Zhou Y.Zhou V.Zhovkovska X.Zhu X.Zhu Z.Zhu V.Zhukov Q.Zou S.Zucchelli D.Zuliani G.Zunica LHCb Collaboration 《Chinese Physics C》 SCIE CAS CSCD 2023年第9期1-13,共13页
A first search for the Ξ_(bc)^(+)J/ψΞ_(c)^(+) decay is performed by the LHCb experiment with a data sample of proton-proton collisions, corresponding to an integrated luminosity of 9 fb−1 recorded at centre-of-mass... A first search for the Ξ_(bc)^(+)J/ψΞ_(c)^(+) decay is performed by the LHCb experiment with a data sample of proton-proton collisions, corresponding to an integrated luminosity of 9 fb−1 recorded at centre-of-mass energies of 7, 8, and 13 TeV. Two peaking structures are seen with a local (global) significance of 4.3(2.8) and 4.1(2.4) standard deviations at masses of 6571 and 6694 MeV/c2, respectively. Upper limits are set on the Ξ+bc baryon production cross-section times the branching fraction relative to that of the B+c→J/ψD+s decay at centre-of-mass energies of 8 and 13 TeV, in the Ξ+bc and in the B+c rapidity and transverse-momentum ranges from 2.0 to 4.5 and 0 to 20GeV/c, respectively. Upper limits are presented as a function of the Ξ+bc mass and lifetime. 展开更多
关键词 QCD B physics charm physics spectroscopy
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Search for the rare decays W^(+)→D_(s)^(+)γ and Z→D^(0)γ at LHCb
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作者 R.Aaij A.S.W.Abdelmotteleb +1069 位作者 C.Abellan Beteta F.Abudinén T.Ackernley B.Adeva M.Adinolfi P.Adlarson H.Afsharnia C.Agapopoulou C.A.Aidala Z.Ajaltouni S.Akar K.Akiba J.Albrecht F.Alessio M.Alexander A.Alfonso Albero Z.Aliouche P.Alvarez Cartelle R.Amalric S.Amato J.L.Amey Y.Amhis L.An L.Anderlini M.Andersson A.Andreianov M.Andreotti D.Andreou D.Ao F.Archilli A.Artamonov M.Artuso E.Aslanides M.Atzeni B.Audurier S.Bachmann M.Bachmayer J.J.Back A.Bailly-reyre P.Baladron Rodriguez V.Balagura W.Baldini J.Baptista de Souza Leite M.Barbetti R.J.Barlow S.Barsuk W.Barter M.Bartolini F.Baryshnikov J.M.Basels G.Bassi B.Batsukh A.Battig A.Bay A.Beck M.Becker F.Bedeschi I.B.Bediaga A.Beiter V.Belavin S.Belin V.Bellee K.Belous I.Belov I.Belyaev G.Benane G.Bencivenni E.Ben-Haim A.Berezhnoy R.Bernet S.Bernet Andres D.Berninghoff H.C.Bernstein C.Bertella A.Bertolin C.Betancourt F.Betti Ia.Bezshyiko S.Bhasin J.Bhom L.Bian M.S.Bieker N.V.Biesuz S.Bifani P.Billoir A.Biolchini M.Birch F.C.R.Bishop 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E.Luppi A.Lusiani K.Lynch X.-R.Lyu L.Ma R.Ma S.Maccolini F.Machefert F.Maciuc I.Mackay V.Macko P.Mackowiak L.R.Madhan Mohan A.Maevskiy D.Maisuzenko M.W.Majewski J.J.Malczewski S.Malde B.Malecki A.Malinin T.Maltsev G.Manca G.Mancinelli C.Mancuso D.Manuzzi C.A.Manzari D.Marangotto J.F.Marchand U.Marconi S.Mariani C.Marin Benito J.Marks A.M.Marshall P.J.Marshall G.Martelli G.Martellotti L.Martinazzoli M.Martinelli D.Martinez Santos F.Martinez Vidal A.Massafferri M.Materok R.Matev A.Mathad V.Matiunin C.Matteuzzi K.R.Mattioli A.Mauri E.Maurice J.Mauricio M.Mazurek M.McCann L.Mcconnell T.H.McGrath N.T.McHugh A.McNab R.McNulty J.V.Mead B.Meadows G.Meier D.Melnychuk S.Meloni M.Merk A.Merli L.Meyer Garcia D.Miao M.Mikhasenko D.A.Milanes E.Millard M.Milovanovic M.-N.Minard A.Minotti T.Miralles S.E.Mitchell B.Mitreska D.S.Mitzel A.Madden R.A.Mohammed R.D.Moise S.Mokhnenko T.Mombacher M.Monk I.A.Monroy S.Monteil M.Morandin G.Morello M.J.Morello J.Moron A.B.Morris A.G.Morris R.Mountain H.Mu 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A.Poluektov N.Polukhina I.Polyakov E.Polycarpo S.Ponce D.Popov S.Popov S.Poslavskii K.Prasanth L.Promberger C.Prouve V.Pugatch V.Puill G.Punzi H.R.Qi W.Qian N.Qin S.Qu R.Quagliani N.V.Raab R.I.Rabadan Trejo B.Rachwal J.H.Rademacker R.Rajagopalan M.Rama M.Ramos Pernas M.S.Rangel F.Ratnikov G.Raven M.Rebollo De Miguel F.Redi J.Reich F.Reiss C.Remon Alepuz Z.Ren P.K.Resmi R.Ribatti A.M.Ricci S.Ricciardi K.Richardson M.Richardson-Slipper K.Rinnert P.Robbe G.Robertson A.B.Rodrigues E.Rodrigues E.Rodriguez Fernandez J.A.Rodriguez Lopez E.Rodriguez Rodriguez D.L.Rolf A.Rollings P.Roloff V.Romanovskiy M.Romero Lamas A.Romero Vidal J.D.Roth M.Rotondo M.S.Rudolph T.Ruf R.A.Ruiz Fernandez J.Ruiz Vidal A.Ryzhikov J.Ryzka J.J.Saborido Silva N.Sagidova N.Sahoo B.Saitta M.Salomoni C.Sanchez Gras I.Sanderswood R.Santacesaria C.Santamarina Rios M.Santimaria E.Santovetti D.Saranin G.Sarpis M.Sarpis A.Sarti C.Satriano A.Satta M.Saur D.Savrina H.Sazak L.G.Scantlebury Smead A.Scarabotto S.Schael S.Scherl 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K.A.Thomson H.Tilquin V.Tisserand S.T'Jampens M.Tobin L.Tomassetti G.Tonani X.Tong D.Torres Machado D.Y.Tou S.M.Trilov C.Trippl G.Tuci A.Tully N.Tuning A.Ukleja D.J.Unverzagt A.Usachov A.Ustyuzhanin U.Uwer A.Vagner V.Vagnoni A.Valassi G.Valenti N.Valls Canudas M.van Beuzekom M.Van Dijk H.Van Hecke E.van Herwijnen C.B.Van Hulse M.van Veghel R.Vazquez Gomez P.Vazquez Regueiro C.Vázquez Sierra S.Vecchi J.J.Velthuis M.Veltri A.Venkateswaran M.Veronesi M.Vesterinen D.Vieira M.Vieites Diaz X.Vilasis-Cardona E.Vilella Figueras A.Villa P.Vincent F.C.Volle D.vom Bruch A.Vorobyev V.Vorobyev N.Voropaev K.Vos C.Vrahas R.Waldi J.Walsh G.Wan C.Wang G.Wang J.Wang J.Wang J.Wang J.Wang M.Wang R.Wang X.Wang Y.Wang Z.Wang Z.Wang Z.Wang J.A.Ward N.K.Watson D.Websdale Y.Wei C.Weisser B.D.C.Westhenry D.J.White M.Whitehead A.R.Wiederhold D.Wiedner G.Wilkinson M.K.Wilkinson I.Williams M.Williams M.R.J.Williams R.Williams F.F.Wilson W.Wislicki M.Witek L.Witola C.P.Wong G.Wormser S.A.Wotton H.Wu J.Wu K.Wyllie Z.Xiang D.Xiao Y.Xie A.Xu J.Xu L.Xu L.Xu M.Xu Q.Xu Z.Xu Z.Xu D.Yang S.Yang X.Yang Y.Yang Z.Yang Z.Yang L.E.Yeomans V.Yeroshenko H.Yeung H.Yin J.Yu X.Yuan E.Zaffaroni M.Zavertyaev M.Zdybal O.Zenaiev M.Zeng C.Zhang D.Zhang L.Zhang S.Zhang S.Zhang Y.Zhang Y.Zhang A.Zharkova A.Zhelezov Y.Zheng T.Zhou X.Zhou Y.Zhou V.Zhovkovska X.Zhu X.Zhu Z.Zhu V.Zhukov Q.Zou S.Zucchelli D.Zuliani G.Zunica LHCb Collaboration 《Chinese Physics C》 SCIE CAS CSCD 2023年第9期14-26,共13页
A search for the rare decays W^(+)→D_(s)^(+)γ and Z→D0γis performed using proton-proton collision data collected by the LHCb experiment at a centre-of-mass energy of 13TeV,corresponding to an integrated luminosity... A search for the rare decays W^(+)→D_(s)^(+)γ and Z→D0γis performed using proton-proton collision data collected by the LHCb experiment at a centre-of-mass energy of 13TeV,corresponding to an integrated luminosity of 2.0fb−1.No significant signal is observed for either decay mode and upper limits on their branching fractions are set using W^(+)→D_(s)^(+)γ and Z→μ+μ−decays as normalization channels.The upper limits are 6.5×10^(−4) and 2.1×10^(−3) at 95% confidence level for the W^(+)→D_(s)^(+)γ and Z→D^(0)γ decay modes,respectively.This is the first reported search for the Z→D^(0)γ decay,while the upper limit on the W+→D+sγbranching fraction improves upon the previous best limit. 展开更多
关键词 W/Z boson rare decay upper limit of branching fraction
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Measurement of integrated luminosities at BESⅢ for data samples at center-of-mass energies between 4.0 and 4.6 GeV
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作者 M.Ablikim M.N.Achasov +561 位作者 P.Adlarson S.Ahmed M.Albrecht R.Aliberti A.Amoroso M.R.An Q.An X.H.Bai Y.Bai O.Bakina R.Baldini Ferroli I.Balossino Y.Ban V.Batozskaya D.Becker K.Begzsuren N.Berger M.Bertani D.Bettoni F.Bianchi J.Bloms 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 W.L.Chang G.Chelkov C.Chen G.Chen H.S.Chen M.L.Chen S.J.Chen T.Chen X.R.Chen X.T.Chen Y.B.Chen Z.J.Chen W.S.Cheng X.Chu G.Cibinetto F.Cossio J.J.Cui H.L.Dai J.P.Dai A.Dbeyssi R.Ede Boer D.Dedovich Z.Y.Deng A.Denig I.Denysenko M.Destefanis F.De Mori Y.Ding J.Dong L.Y.Dong M.Y.Dong X.Dong S.X.Du P.Egorov Y.L.Fan J.Fang S.S.Fang W.X.Fang Y.Fang R.Farinelli L.Fava F.Feldbauer G.Felici C.Q.Feng J.H.Feng K Fischer M.Fritsch C.Fritzsch C.D.Fu H.Gao Y.N.Gao Yang Gao S.Garbolino I.Garzia P.T.Ge C.Geng E.M.Gersabeck A Gilman K.Goetzen L.Gong W.X.Gong W.Gradl M.Greco M.H.Gu C.Y Guan A.Q.Guo L.B.Guo R.P.Guo Y.P.Guo A.Guskov 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 M.Himmelreich T.Holtmann G.Y.Hou Y.R.Hou Z.L.Hou H.M.Hu J.F.Hu T.Hu Y.Hu G.S.Huang K.X.Huang L.Q.Huang L.Q.Huang X.T.Huang Y.P.Huang Z.Huang T.Hussain N Husken W.Imoehl M.Irshad J.Jackson S.Jaeger S.Janchiv Q.Ji Q.P.Ji X.B.Ji X.L.Ji Y.Y.Ji Z.K.Jia H.B.Jiang S.S.Jiang X.S.Jiang Y.Jiang J.B.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing T.Johansson N.Kalantar-Nayestanaki X.S.Kang R.Kappert M.Kavatsyuk B.C.Ke I.K.Keshk A.Khoukaz P.Kiese R.Kiuchi R.Kliemt L.Koch O.B.Kolcu B.Kopf M.Kuemmel M.Kuessner A.Kupsc W.Kuhn J.J.Lane J.S.Lange P.Larin A.Lavania L.Lavezzi Z.H.Lei H.Leithoff M.Lellmann T.Lenz C.Li C.Li C.H.Li Cheng Li D.M.Li F.Li G.Li H.Li H.Li H.B.Li H.J.Li H.N.Li J.Q.Li J.S.Li J.W.Li Ke Li L.J Li L.K.Li Lei Li M.H.Li P.R.Li S.X.Li S.Y.Li T.Li W.D.Li W.G.Li X.H.Li X.L.Li Xiaoyu Li Z.Y.Li H.Liang H.Liang H.Liang Y.F.Liang Y.T.Liang G.R.Liao L.Z.Liao J.Libby A.Limphirat C.X.Lin D.X.Lin T.Lin B.J.Liu C.X.Liu D.Liu F.h.liu Fang Liu Feng Liu G.M.Liu h.liu H.M.Liu Huanhuan Liu Huihui Liu J.B.Liu J.L.Liu J.Y.Liu K.Liu K.Y.Liu Ke Liu L.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.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.L.Ma L.L.Ma M.M.Ma Q.M.Ma R.Q.Ma R.T.Ma X.Y.Ma Y.Ma F.E.Maas M.Maggiora S.Maldaner S.Malde Q.A.Malik 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 N.Yu.Muchnoi H.Muramatsu Y.Nefedov F.Nerling I.B.Nikolaev Z.Ning S.Nisar Y.Niu S.L.Olsen Q.Ouyang S.Pacetti X.Pan Y.Pan A.Pathak A.Pathak M.Pelizaeus H.P.Peng K.Peters J.Pettersson J.L.Ping R.G.Ping S.Plura S.Pogodin R.Poling V.Prasad F.Z.Qi H.Qi H.R.Qi M.Qi T.Y.Qi S.Qian W.B.Qian Z.Qian C.F.Qiao J.J.Qin L.Q.Qin X.P.Qin X.S.Qin Z.H.Qin J.F.Qiu S.Q.Qu S.Q.Qu K.H.Rashid C.F.Redmer K.J.Ren A.Rivetti V.Rodin M.Rolo G.Rong Ch.Rosner S.N.Ruan H.S.Sang A.Sarantsev Y.Schelhaas C.Schnier 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 X.Y.Shen B.-A.Shi H.C.Shi J.Y.Shi R.S.Shi X.Shi X.D Shi J.J.Song W.M.Song Y.X.Song S.Sosio S.Spataro F.Stieler K.X.Su P.P.Su Y.-J.Su G.X.Sun H.Sun H.K.Sun J.F.Sun L.Sun S.S.Sun T.Sun W.Y.Sun X Sun Y.J.Sun Y.Z.Sun Z.T.Sun Y.H.Tan Y.X.Tan C.J.Tang G.Y.Tang J.Tang L.Y Tao Q.T.Tao J.X.Teng V.Thoren W.H.Tian Y.Tian I.Uman B.Wang B.L.Wang D.Y.Wang F.Wang H.J.Wang H.P.Wang K.Wang L.L.Wang M.Wang M.Z.Wang Meng Wang S.Wang T.Wang T.J.Wang W.Wang W.H.Wang W.P.Wang X.Wang X.F.Wang X.L.Wang Y.D.Wang Y.F.Wang Y.H.Wang Y.Q.Wang Ying Wang Z.Wang Z.Y.Wang Ziyi Wang D.H.Wei F.Weidner S.P.Wen D.J.White U.Wiedner G.Wilkinson M.Wolke L.Wollenberg J.F.Wu L.H.Wu L.J.Wu X.Wu X.H.Wu Y.Wu Z.Wu L.Xia T.Xiang D.Xiao H.Xiao S.Y.Xiao Y.L.Xiao Z.J.Xiao 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 Q.J.Xu S.Y.Xu X.P.Xu Y.C.Xu F.Yan L.Yan W.B.Yan W.C.Yan H.J.Yang H.L.Yang H.X.Yang L.Yang S.L.Yang Tao Yang Y.X.Yang Yifan Yang M.Ye M.H.Ye J.H.Yin Z.Y.You B.X.Yu C.X.Yu G.Yu T.Yu C.Z.Yuan L.Yuan S.C.Yuan X.Q.Yuan Y.Yuan Z.Y.Yuan C.X.Yue A.A.Zafar F.R.Zeng X.Zeng Y.Zeng Y.H.Zhan A.Q.Zhang B.L.Zhang B.X.Zhang D.H.Zhang G.Y.Zhang H.Zhang H.H.Zhang H.H.Zhang H.Y.Zhang J.L.Zhang J.Q.Zhang J.W.Zhang J.X.Zhang J.Y.Zhang J.Z.Zhang Jianyu Zhang Jiawei Zhang L.M.Zhang L.Q.Zhang Lei Zhang P.Zhang Q.Y.Zhang Shulei Zhang X.D.Zhang X.M.Zhang X.Y.Zhang X.Y.Zhang Y.Zhang Y.T.Zhang Y.H.Zhang Yan Zhang Yao Zhang Z.H.Zhang Z.Y.Zhang Z.Y.Zhang G.Zhao J.Zhao J.Y.Zhao J.Z.Zhao Lei Zhao Ling Zhao M.G.Zhao Q.Zhao S.J.Zhao Y.B.Zhao Y.X.Zhao Z.G.Zhao A.Zhemchugov B.Zheng J.P.Zheng Y.H.Zheng B.Zhong C.Zhong X.Zhong H.Zhou L.P.Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou Y.Z.Zhou J.Zhu K.Zhu K.J.Zhu L.X.Zhu S.H.Zhu T.J.Zhu W.J.Zhu Y.C.Zhu Z.A.Zhu B.S.Zou J.H.Zou Y.T.Gu H.B.Liu 《Chinese Physics C》 SCIE CAS CSCD 2022年第11期53-63,共11页
The integrated luminosities of data samples collected in the BESⅢ experiment in 2016-2017 at centerof-mass energies between 4.19 and 4.28 GeV are measured with a precision better than 1% by analyzing large-angle Bhab... The integrated luminosities of data samples collected in the BESⅢ experiment in 2016-2017 at centerof-mass energies between 4.19 and 4.28 GeV are measured with a precision better than 1% by analyzing large-angle Bhabha scattering events.The integrated luminosities of old datasets collected in 2010-2014 are updated by considering corrections related to detector performance,offsetting the effect of newly discovered readout errors in the electromagnetic calorimeter,which can haphazardly occur. 展开更多
关键词 integrated luminosity e^(+)e^(-)annihilation Bhabha scattering
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