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三轴形变核^(131)Ba中的奇异集体激发模式
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作者 韦锐 周厚兵 +34 位作者 王思成 丁兵 强赟华 贾晨旭 陈红星 郭松 C.M.Petrache D.Mengoni A.Astier E.Dupont 吕冰锋 D.Bazzacco A.Boso A.Goasduff F.Recchia D.Testov F.Galtarossa G.Jaworski D.R.Napoli S.Riccetto M.Siciliano J.J.Valiente-Dobon C.Andreoiu F.H.Garcia K.Ortner K.Whitmore A.Ataç-Nyberg T.Bäck B.Cederwall E.A.Lawrie I.Kuti D.Sohler T.Marchlewski J.Srebrny A.Tucholski 《物理学报》 SCIE EI CAS CSCD 北大核心 2024年第11期89-100,共12页
利用意大利Legnaro实验室串列静电加速器提供的65 MeV^(13)C束流与122Sn靶的熔合蒸发反应布居了^(131)Ba的高自旋态,并搭建了新的能级纲图.新的能级纲图由15条转动带组成,包括三对手征双重带,其中两对正宇称手征带为赝自旋-手征四重带.... 利用意大利Legnaro实验室串列静电加速器提供的65 MeV^(13)C束流与122Sn靶的熔合蒸发反应布居了^(131)Ba的高自旋态,并搭建了新的能级纲图.新的能级纲图由15条转动带组成,包括三对手征双重带,其中两对正宇称手征带为赝自旋-手征四重带.正负宇称手征带通过一系列增强的E1跃迁连接,表明它们之间存在八极关联.在低自旋区域搭建了一条新的转动带,通过一系列γ跃迁向νh1_(1/2)晕带退激.这种能级结构与摇摆带相似,但基于现有的实验证据还难以将它确认为摇摆带,不能排除其他集体激发机制,如γ振动的影响. 展开更多
关键词 高自旋态 手征带 赝自旋 八极关联 摇摆运动
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Determinants of saturation magnetic flux density in Fe-based metallic glasses:insights from machine-learning models 被引量:1
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作者 Jie Xiong Bo-Wen Bai +1 位作者 Hao-Ran Jiang Angeles Faus-Golfe 《Rare Metals》 SCIE EI CAS CSCD 2024年第10期5256-5267,共12页
Fe-based metallic glasses have garnered significant attention due to their low coercivity force and core loss.Enhancing the saturation magnetic flux density(Bs)of Fe-based metallic glasses is crucial for their industr... Fe-based metallic glasses have garnered significant attention due to their low coercivity force and core loss.Enhancing the saturation magnetic flux density(Bs)of Fe-based metallic glasses is crucial for their industry applications.This work constructed a dataset comprising330 training data and 157 test data.The support vector regression model surpassed the tree-based ensemble models in the test set and demonstrated comparable accuracy to the tree-based ensemble models in the training set.Additionally,we proposed an indicator for Bsbased on symbolic regression.This newly proposed indicator exhibits a Pearson correlation coefficient exceeding 0.92 with Bs.The present work provides a simple and accurate formula for predicting the Bsof Fe-based amorphous alloys,demonstrating the effectiveness of machine learning approaches in discovering novel soft magnetic materials. 展开更多
关键词 Saturation magnetic flux density Fe-based metallic glasses Machine learning Symbolic regression
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Charge resolution in the isochronous mass spectrometry and the mass of ^(51)Co 被引量:4
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作者 Xu Zhou Meng Wang +25 位作者 Yu-Hu Zhang Hu-Shan Xu You-Jin Yuan Jian-Cheng Yang Yu.A.Litvinov S.A.Litvinov Bo Mei Xin-Liang Yan Xing Xu Peng Shuai Yuan-Ming Xing Rui-Jiu Chen Xiang-Cheng Chen Chao-Yi Fu Qi Zeng Ming-Ze Sun Hong-Fu Li Qian Wang Tong Bao Min Zhang Min Si Han-Yu Deng Ming-Zheng Liu Ting Liao Jin-Yang Shi Yu-Nan Song 《Nuclear Science and Techniques》 SCIE EI CAS CSCD 2021年第4期30-37,共8页
Isochronous mass spectrometry(IMS)of heavyion storage rings is a powerful tool for the mass measurements of short-lived nuclei.In IMS experiments,masses are determined through precision measurements of the revolution ... Isochronous mass spectrometry(IMS)of heavyion storage rings is a powerful tool for the mass measurements of short-lived nuclei.In IMS experiments,masses are determined through precision measurements of the revolution times of the ions stored in the ring.However,the revolution times cannot be resolved for particles with nearly the same mass-to-charge(m/q)ratios.To overcome this limitation and to extract the accurate revolution times for such pairs of ion species with very close m/q ratios,in our early work on particle identification,we analyzed the amplitudes of the timing signals from the detector based on the emission of secondary electrons.Here,the previous data analysis method is further improved by considering the signal amplitudes,detection efficiencies,and number of stored ions in the ring.A sensitive Z-dependent parameter is introduced in the data analysis,leading to a better resolution of ^(34)Ar^(18+) and ^(51)Co^(27+) with A/Z=17/9.The mean revolution times of ^(34)Ar^(18+) and ^(51)Co^(27+) are deduced,although their time difference is merely 1.8 ps.The uncorrected,overlapped peak of these ions has a full width at half maximum of 7.7 ps.The mass excess of ^(51)Co was determined to be-27;332e41T keV,which is in agreement with the previous value of-27;342e48T keV. 展开更多
关键词 Isochronous mass spectrometry Charge resolution Signal amplitude Micro-channel plate ^(51)Co
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Continuous-wave optical enhancement cavity with 30-kW average power
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作者 柳兴 陆心怡 +6 位作者 王焕 颜立新 李任恺 黄文会 唐传祥 Ronic Chiche Fabian Zomer 《Chinese Physics B》 SCIE EI CAS CSCD 2023年第3期258-261,共4页
Optical enhancement cavity(OEC)is a powerful tool for fundamental research and diagnostics.In this paper,the progress of a continuous-wave OEC to realize of megawatt cavity for a novel light source based on a steady-s... Optical enhancement cavity(OEC)is a powerful tool for fundamental research and diagnostics.In this paper,the progress of a continuous-wave OEC to realize of megawatt cavity for a novel light source based on a steady-state microbunching(SSMB)mechanism,is reported.After efficiently suppressing all external noise and optimizing the alignment,mode-matching,and polarization matching,stable and long-term locking is achieved with the help of two feedback loops.The modal instability phenomenon caused by the surface thermoelastic deformation is observed.A pair of D-shape mirrors are utilized to remove the high-order modes.Finally,an intra-cavity average power of 30 kW is reached. 展开更多
关键词 optical enhancement cavity continuous-wave laser modal instability high power cavity
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Nucleus++:a new tool bridging AME and NuBAsE for advancing nuclear data analysis
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作者 Jin-Yang Shi Wen-Jia Huang +6 位作者 Meng Wang Xin-Liang Yan David Lunney Georges Audi Filip GKondev Sarah Naimi Rikel Chakma 《Nuclear Science and Techniques》 SCIE EI CAS CSCD 2024年第10期233-238,共6页
The newly developed software,Nucleus++,is an advanced tool for displaying basic nuclear physics properties from NubAsE and integrating comprehensive mass information for each nuclide from Atomic Mass Evaluation.Additi... The newly developed software,Nucleus++,is an advanced tool for displaying basic nuclear physics properties from NubAsE and integrating comprehensive mass information for each nuclide from Atomic Mass Evaluation.Additionally,it allows users to compare experimental nuclear masses with predictions from different mass models.Building on the success and learning experiences of its predecessor,Nucleus,this enhanced tool introduces improved functionality and compatibility.With its user-friendly interface,Nucleus++was designed as a valuable tool for scholars and practitioners in the field of nuclear science.This article offers an in-depth description of Nucleus++,highlighting its main features and anticipated impacts on nuclear science research. 展开更多
关键词 Nucleus++ Nuclear physics properties NUBASE AME Nuclear science Software design
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^(3)S_(1)–^(3)D_(1) coupled channel Λ_(c)N interactions:chiral effective field theory versus lattice QCD
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作者 Jing Song Yang Xiao +2 位作者 Zhi-Wei Liu Kai-Wen Li Li-Sheng Geng 《Communications in Theoretical Physics》 SCIE CAS CSCD 2023年第1期86-95,共10页
We study the lattice QCDΛ_(c)N phase shifts for the^(3)S_(1)-^(3)D_(1)coupled channel using both the leading order covariant chiral effective theory and the next-to-leading order non-relativistic chiral effective fie... We study the lattice QCDΛ_(c)N phase shifts for the^(3)S_(1)-^(3)D_(1)coupled channel using both the leading order covariant chiral effective theory and the next-to-leading order non-relativistic chiral effective field theory(ChEFT).We show that although it is possible to describe simultaneously the^(3)S_(1)and^(3)D_(1)phase shifts and the inelasticityη_(1),the fitted energy range is quite small,only up to E_(c.m.)=5 MeV.This raises concerns regarding the consistency between leading/next-to-leading order ChEFT and the lattice QCD simulations. 展开更多
关键词 Λ_(c)N interaction covariant ChEFT lattice QCD
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A Fast Radio Burst Backend for the Tianlai Dish Pathfinder Array
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作者 Zijie Yu Furen Deng +11 位作者 Shijie Sun Chenhui Niu Jixia Li Fengquan Wu Wei-Yang Wang Yougang Wang Hui Feng Lin Shu Jie Hao Reza Ansari Albert Stebbins Xuelei Chen 《Research in Astronomy and Astrophysics》 SCIE CAS CSCD 2022年第12期211-223,共13页
The Tianlai Dish Pathfinder Array is a radio interferometer array consisting of 16 six-meter dish antennas.The original digital backend integration time is at the seconds level,designed for H I intensity mapping exper... The Tianlai Dish Pathfinder Array is a radio interferometer array consisting of 16 six-meter dish antennas.The original digital backend integration time is at the seconds level,designed for H I intensity mapping experiment.A new digital backend with millisecond response is added to enable it to search for fast radio burst during its observations.The design and calibration of this backend,and the real time search pipeline for it are described in this paper.It is capable of forming 16 digital beams for each linear polarization,covering an area of 19.6 square degrees.The search pipeline is capable of searching for,recording and classifying FRBs automatically in real time.In commissioning,we succeeded in capturing the signal pulses from the pulsars PSR B0329+54 and B2021+51. 展开更多
关键词 instrumentation:miscellaneous techniques:interferometric telescopes radio continuum:general (stars:)pulsars:general
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The FRB-searching Pipeline of the Tianlai Cylinder Pathfinder Array
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作者 Zijie Yu Furen Deng +14 位作者 Shijie Sun Chenhui Niu Jixia Li Fengquan Wu Wei-Yang Wang Yougang Wang Shifan Zuo Lin Shu Jie Hao Xiaohui Liu Reza Ansari Ue-Li Pen Albert Stebbins Peter Timbie Xuelei Chen 《Research in Astronomy and Astrophysics》 SCIE CAS CSCD 2024年第8期113-132,共20页
This paper presents the design,calibration,and survey strategy of the Fast Radio Burst(FRB)digital backend and its real-time data processing pipeline employed in the Tianlai Cylinder Pathfinder Array.The array,consist... This paper presents the design,calibration,and survey strategy of the Fast Radio Burst(FRB)digital backend and its real-time data processing pipeline employed in the Tianlai Cylinder Pathfinder Array.The array,consisting of three parallel cylindrical reflectors and equipped with 96 dual-polarization feeds,is a radio interferometer array designed for conducting drift scans of the northern celestial semi-sphere.The FRB digital backend enables the formation of 96 digital beams,effectively covering an area of approximately 40 square degrees with the 3 dB beam.Our pipeline demonstrates the capability to conduct an automatic search of FRBs,detecting at quasi-realtime and classifying FRB candidates automatically.The current FRB searching pipeline has an overall recall rate of88%.During the commissioning phase,we successfully detected signals emitted by four well-known pulsars:PSR B0329+54,B2021+51,B0823+26,and B2020+28.We report the first discovery of an FRB by our array,designated as FRB 20220414A.We also investigate the optimal arrangement for the digitally formed beams to achieve maximum detection rate by numerical simulation. 展开更多
关键词 instrumentation interferometers-methods data analysis-(stars )pulsars general-telescopes
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Discovery of the New Isotope^(251)Lr
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作者 Huang Tianheng D.Seweryniak +28 位作者 B.B.Back P.Bender M.P.Carpenter P.Chowdhury R.M.Clark P.Copp X.-T.He R.D.Herzberg D.Ho H.Jayatissa T.L.Khoo F.G.Kondev G.Morgan Ch.Morse A.Korichi T.Lauritsen C.Muller-Gatermann D.Potterveld W.Reviol A.Rogers S.Saha G.Savard K.Sharma S.Stolze S.Waniganeththi G.Wilson J.Wu Y.-F.Xu S.Zhu 《IMP & HIRFL Annual Report》 2022年第1期38-38,共1页
The products of the^(203,205)Ti(^(50)Ti,2n)fusion-evaporation reactions were studied by using the recently commissioned Argonne Gas-Filled Analyzer(AGFA)at Argonne National Laboratory.
关键词 2n Argonne
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Candidate Revolving Chiral Doublet Bands in^(119)Cs
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作者 Zheng Kuankuan Costel Petrache +32 位作者 Zhang Zhenhua Alain Astier Lv Bingfeng Paul Greenlees Tuomas Grahn Rauno Julin Sanna Juutinen Minna Luoma Jari Ojala Janne Pakarinen Juho Partanen Paavo Rahkila Panu Ruotsalainen Mikael Sandzelius Jan Saren Holly Tann Juha Uusitalo George Zimba Bo Cederwall Ozge Aktas Aysegul Ertoprak Zhang Wei Guo Song Liu Minliang Zhou Xiaohong Istvan Kuti B.M.Nyako D.Sohler J.Timar Corina Andreoiu Maria Doncel David Joss Robert Page 《IMP & HIRFL Annual Report》 2022年第1期32-33,共2页
The chiral bands built on a con guration with only protons in the transient backbending regime was also observed for the rst time in^(119)Cs^([1]).One newly observed band(Band 9)which is nearly degenerate to the stron... The chiral bands built on a con guration with only protons in the transient backbending regime was also observed for the rst time in^(119)Cs^([1]).One newly observed band(Band 9)which is nearly degenerate to the strongly-coupled g9=2[404]9=2^(+)band of 119Cs was identi ed.It exhibits a backbending similar to that of known band(Band 8),at nearly constant rotation frequency. 展开更多
关键词 BENDING ROTATION DEGENERATE
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Conceptual design report of the Super Tau-Charm Facility:the accelerator
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作者 Xiao-Cong Ai Liu-Pan An +451 位作者 Shi-Zhong An Yu Bai Zheng-He Bai Olga Bakina Jian-Cong Bao Varvara Batozskaya Anastasios Belias Maria Enrica Biagini Li-Gong Bian Denis Bodrov Anton Bogomyagkov Manuela Boscolo Igor Boyko Ze-Xin Cao Serkant Cetin Marina Chadeeva Ming-Xuan Chang Qin Chang Dian-Yong Chen Fang-Zhou Chen Hai Chen Hua-Xing Chen Jin-Hui Chen Long Chen Long-Bin Chen Qi Chen Qu-Shan Chen Shao-Min Chen Wei Chen Ying Chen Zhi Chen Shan Cheng Si-Bo Cheng Tong-Guang Cheng Lian-Rong Dai Ling-Yun Dai Xin-Chen Dai Achim Denig Igor Denisenko Denis Derkach Heng-Tong Ding Ming-Hui Ding Xiao Ding Liao-Yuan Dong Yong Du Prokhor Egorov Kuan-Jun Fan Si-Yuan Fan Shuang-Shi Fang Zhu-Jun Fang Song Feng Xu Feng Hai-Bing Fu Jun Gao Yuan-Ning Gao Zi-Han Gao Cong Geng Li-Sheng Geng Hai-Liang Gong Jia-Ding Gong Li Gong Shao-Kun Gong Sergi Gonzàlez-Solís Bo-Xing Gou Duan Gu Hao Guo Jun Guo Teng-Jun Guo Xin-Heng Guo Yu-Hui Guo Yu-Ping Guo Zhi-Hui Guo Selcuk Haciomeroglu Eiad Hamwi Cheng-Dong Han Ting-Ting Han Xi-Qing Hao Chong-Chao He Ji-Bo He Tian-Long He Xiao-Gang He Masahito Hosaka Kai-Wen Hou Zhi-Long Hou Dong-Dong Hu Hai-Ming Hu Hao Hu Qi-Peng Hu Tong-Ning Hu Xiao-Cheng Hu Yu Hu Zhen Hu Da-Zhang Huang Fei Huang Guang-Shun Huang Liang-Sheng Huang Peng-Wei Huang Rui-Xuan Huang Xing-Tao Huang Xue-Lei Huang Zhi-Cheng Huang Wang Ji Peng-Kun Jia Sen Jia Ze-Kun Jia Hong-Ping Jiang Hou-Bing Jiang Jian-Bin Jiao Ming-Jie Jin Su-Ping Jin Yi Jin Daekyoung Kang Xian-Wei Kang Xiao-Lin Kang Leonid Kaptari Onur Bugra Kolcu Ivan Koop Evgeniy Kravchenko Yury Kudenko Meike Küßner Yong-Bin Leng Eugene Levichev Chao Li Chun-Yuan Li Chun-Hua Li Hai Tao Li Hai-Bo Li Hang-Zhou Li Heng-Ne Li Hong-Lei Li Hui-Jing Li Hui-Lin Li Jia-Rong Li Jin Li Lei Li Min Li Pei-Rong Li Pei-Lian Li Ren-Kai Li Sang-Ya Li Shu Li Teng Li Tian-You Li Wei-Wei Li Wen-Jun Li Xin Li Xin-Qiang Li Xin-Bai Li Xuan Li Xun-Feng Li Yan-Feng Li Ya-Xuan Li Ying Li Yu-Bo Li Jian Liang Xiao Liang Yu Liang Ze-Rui Liang Chuang-Xin Lin De-Xu Lin Ting Lin Yu-Gen Lin Chao Liu Chao Liu Chia-Wei Liu Gang-Wen Liu Hang Liu Hong-Bang Liu Jian-Bei Liu Jian-Dang Liu Lang-Tian Liu Liang-Chen Liu Ming-Yi Liu Shu-Bin Liu Tao Liu Tian-Bo Liu Xiang Liu Xiao-Yu Liu Xin Liu Xu-Yang Liu Yan-Rui Liu Yan-Lin Liu Yan-Wen Liu Yi Liu Yuan Liu Zhan-Wei Liu Zhao-Feng Liu Zhi-Qing Liu Zi-Rui Liu Zuo-Wei Liu Cai-Dian Lu Miao-Ran Lu Peng-Cheng Lu Yu Lu Qing Luo Tao Luo Tao Luo Xiao-Feng Luo Hui-Hui Lv Shuo-Tian Lyu Xiao-Rui Lyu Bo-Qiang Ma Cheng-Long Ma Shao-Hang Ma Teng Ma Wen-Bin Ma Yu Meng Meng-Xu Fan Xue-Ce Miao Mauro Migliorati Catia Milardi Taisiya Mineeva Yi-Hao Mo Hector Gisbert Mullor Elaf Musa Satoshi Nakamura Alexey Nefediev Yuan-Cun Nie Kazuhito Ohmi MPadmanath Pavel Pakhlov Jian Pang Emilie Passemar Guo-Xi Pei Hua Pei Hai-Ping Peng Liang Peng Rong-Gang Ping Bernard Pire Vindhyawasini Prasad Bin-Bin Qi Zhi-Jun Qi Yi Qian Cong-Feng Qiao Jia-Jia Qin Long-Yu Qin Qin Qin Xiao-Shuai Qin Fedor Ratnikov Craig Roberts Antonio Rodríguez-Sánchez Yury Rogovsky Platon Rogozhin Pablo Roig Man-Qi Ruan Jorge Segovia Feng-Lei Shang Lei Shang Jian-Feng Shangguan Ding-Yu Shao Ming Shao Zhuo-Xia Shao Cheng-Ping Shen Hong-Fei Shen Xiao-Min Shen Zhong-Tao Shen Cai-Tu Shi Jia-Lei Shi Rui-Xiang Shi Yu-Kun Shi Zong-Guo Si Luiz Vale Silva Mikhail Skamarokha Jun-Chao Su Guang-Bao Sun Jun-Feng Sun Kun Sun Li Sun Ming-Kai Sun Rui Sun Xu-Lei Sun Jing-Yu Tang Yin-Gao Tang Ze-Bo Tang Wei Tao Valery Telnov Jia-Xiu Teng Yuriy Tikhonov Cheng-Ying Tsai Timofey Uglov Vincenzo Vagnoni German Valencia Guan-Yue Wan An-Xin Wang Bin Wang Cheng-Zhe Wang En Wang Hong-Jin Wang Jia Wang Jie Wang Jun-Zhang Wang Lei Wang Lei Wang Lin Wang Qian Wang Qian Wang Sheng-Quan Wang Sheng-Yuan Wang Shi-Kang Wang Wei Wang Wei-Ping Wang Xiang-Peng Wang Xia-Yu Wang Xiong-Fei Wang Ya-Qian Wang Yu-Ming Wang Yu-Hao Wang Zeren Simon Wang Zhi Wang Zhi-Gang Wang Zhi-Yong Wang Zi-Yu Wang Zi-Rui Wang Bing-Feng Wei Shao-Qing Wei Shu-Yi Wei Xiao-Min Wei Ya-Jing Wei Ye-Long Wei Ulrich Wiedner Jia-Jun Wu Jun Wu Qun Wu Sang Wu Xin Wu Xing-Gang Wu Xuan Wu Yong-Cheng Wu Yu-Sheng Wu Lei Xia Zhi-Gang Xiao Chun-Jie Xie Kai-Bo Xie Zi-Yu Xiong Ji Xu Lai-Lin Xu Shu-Sheng Xu Xin Xu Yue Xu Liang Yan Wen-Biao Yan Xue-Qing Yan Chi Yang Hai-Jun Yang Hong-Tao Yang Jun Yang Peng-Hui Yang Shuai Yang Tao Yang Wei-Hua Yang Xing-Hua Yang Xue-Ting Yang Yue-Ling Yang Zhen-Wei Yang Zhong-Juan Yang De-Liang Yao Zao-Chen Ye Kai Yi Li Yi Li-Xin Yin Zheng-Yun You Chen Yu Ze Yu Jing Yuan You-Jin Yuan Nefedov Yury Yi-Feng Zeng Wang-Mei Zha Ai-Lin Zhang Ding-Yue Zhang Guang-Yi Zhang Guo-Heng Zhang Hai-Yan Zhang Hao-Ran Zhang Hong-Hao Zhang Hui-Bin Zhang Jia-Lian Zhang Jian-Rong Zhang Jian-Hui Zhang Jian-Yu Zhang Jie-Lei Zhang Lei Zhang Liang Zhang Ling-Hua Zhang Lin-Hao Zhang Ning Zhang Qiu-Yan Zhang Quan-Zheng Zhang Rui Zhang Rui-Yang Zhang Shao-Ru Zhang Sheng-Hui Zhang Shu-Lei Zhang Wen-Chao Zhang Xiao-Yang Zhang Xiao-Ming Zhang Xiao-Tao Zhang Xin Zhang Xin-Hui Zhang Yan-Xi Zhang Ya-Teng Zhang Yi-Hao Zhang Yi-Fei Zhang Yu Zhang Yu Zhang Yu-Mei Zhang Zhen-Yu Zhang Zhi-Qing Zhang Zhi-Cai Zhang Jia-Yao Zhao Ming-Gang Zhao Qiang Zhao Rui-Guang Zhao Yang-Cheng Zhao Ze-Xuan Zhao Zheng-Guo Zhao Alexey Zhemchugov Bo Zheng Jing-Xin Zheng Liang Zheng Ran Zheng Xu-Chang Zheng Yang-Heng Zheng Bin Zhong Dai-Cui Zhou De-Min Zhou Hang Zhou Hao Zhou Jian Zhou Jian-Xin Zhou Qin-Song Zhou Shi-Yu Zhou Xiang Zhou Xiao-Kang Zhou Xiao-Rong Zhou Ya-Jin Zhou Yi Zhou Yi-Mei Zhou Ze-Ran Zhou Bing Zhu Jing-Yu Zhu Jing-Ya Zhu Lin Zhu Rui-Lin Zhu Xing-Hao Zhu Ying-Chun Zhu Zian Zhu Mikhail Zobov Yang Zong Bing-Song Zou Ye Zou Jian Zu 《Nuclear Science and Techniques》 2025年第12期8-177,共170页
Electron-positron colliders operating in the GeV center-of-mass range,or tau-charm energy region,have been proved to enable competitive frontier research due to several unique features.With the progress of high-energy... Electron-positron colliders operating in the GeV center-of-mass range,or tau-charm energy region,have been proved to enable competitive frontier research due to several unique features.With the progress of high-energy physics in the last two decades,a new-generation Tau-Charm factory,called the Super Tau-Charm Facility(STCF),has been actively promoted by the particle physics community in China.STCF has the potential to address fundamental questions such as the essence of color confinement and the matter-antimatter asymmetry within the next decades.The main design goals of the STCF are a center-of-mass energy ranging from 2 to 7 GeV and a luminosity surpassing 5×10^(34)cm^(−2)s^(−1)that is optimized at a center-of-mass energy of 4 GeV,which is approximately 50 times that of the currently operating Tau-Charm factory-BEPCII.The STCF accelerator has two main parts:a double-ring collider with a crab-waist collision scheme and an injector that provides top-up injections for both electron and positron beams.As a typical third-generation electron-positron circular collider,the STCF accelerator faces many challenges in both accelerator physics and technology.In this paper,the conceptual design of the STCF accelerator complex is presented,including the ongoing efforts and plans for technological research and develop-ment,as well as the required infrastructure.The STCF project aims to secure support from the Chinese central government for its construction during the 15th Five-Year Plan(2026-2030). 展开更多
关键词 Third-generation electron-positron collider Super high-luminosity Tau-charm physics Crab-waist collision scheme Touschek lifetime
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Schottky detection techniques for ultra-rare short-lived ions in heavy-ion storage rings
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作者 M.S.Sanjari Yu.A.Litvinov +10 位作者 G.W.Hudson-Chang S.Naimi D.Dmytriiev J.Glorius E.Menz T.Ohnishi Zs.Podolyak Th.Stöhlker T.Yamaguchi Y.Yamaguchi A.Yano 《Chinese Physics C》 2025年第8期202-206,共5页
Non-destructive Schottky detectors are indispensable devices widely used in experiments at heavy-ion storage rings.In particular,they can be used to accurately determine the masses and lifetimes of short-lived exotic ... Non-destructive Schottky detectors are indispensable devices widely used in experiments at heavy-ion storage rings.In particular,they can be used to accurately determine the masses and lifetimes of short-lived exotic nuclear species.Single-ion sensitivity-which is the highest level of sensitivity-has been regularly achieved in the past by utilizing resonant cavity detectors.Recent designs and analysis methods aim to push the limits of measurement accuracy by increasing the dimensionality of the acquired data,namely,the position of the particle as well as the phase difference between several detectors.This paper describes current methods and future perspectives for Schottky detection techniques,with a focus on their application to mass and lifetime measurements of the most rare and simultaneously short-lived radio nuclides. 展开更多
关键词 heavy ion storage rings mass spectroscopy lifetime measurement rare isotopes highly charged ions instrumentation
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Improvements of time-of-flight detector utilizing a thin foil and crossed static electric and magnetic fields
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作者 Tetsuaki Moriguchi Momo Mukai +31 位作者 Naoto Kaname Akira Ozawa Shinji Suzuki Yasushi Abe Hiroki Arakawa Tomoya Fujii Daiki Hamakawa Sakumi Harayama Shun Hosoi Yasuto Inada Kumi Inomata Reo Kagesawa Daisuke Kajiki Daiki Kamioka Masanori Kanda Atsushi Kitagawa Takaaki Kobayashi Daisuke Nagae Sarah Naimi Kunimitsu Nishimuro Shunichiro Omika Misaki Otsu Mamoru Sakaue Shinji Sato Hibiki Seki Naru Shinozaki Takeshi Suzuki Keisuke Tomita Takayuki Yamaguchi Yoshitaka Yamaguchi Asahi Yano Kenjiro Yokota 《Chinese Physics C》 2025年第10期209-213,共5页
We developed a time-of-flight(TOF)detector with a thin foil for mass measurements of unstable nuclei using the Rare-RI Ring at the RIKEN RI beam factory.Compared to the previous design,the developed TOF detector emplo... We developed a time-of-flight(TOF)detector with a thin foil for mass measurements of unstable nuclei using the Rare-RI Ring at the RIKEN RI beam factory.Compared to the previous design,the developed TOF detector employed modified electrodes,and its static electric and magnetic fields were reduced.We improved the detection efficiency and stability of operation.Its specification and design were finally fixed for mass measurements.We also developed a position-sensitive detector based on the principles of the TOF detector.This study utilized larger microchannel plate(MCP)detectors than those of the prototype.By improving acceptance,we demonstrated the performance of the position-sensitive detector with very low material thickness. 展开更多
关键词 Mass measurement Time-of-flight detector MCP Position-sensitive detector
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Development status of efficiency improvement at the Rare-RI Ring facility
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作者 Y.Yamaguchi A.Yano +22 位作者 T.Ohnishi Y.Abe N.Chandrakumar G.Hudson-Chang N.Imai Y.Kikuchi N.Kitamura R.Kojima J.Li T.Moriguchi D.Nagae S.Naimi S.Nishizawa A.Ozawa F.Suzaki K.Takiura N.Tomioka R.Tuchiya M.Wakasugi K.Watanabe T.Yamaguchi R.Yokoyama H.Zhang 《Chinese Physics C》 2025年第9期134-140,共7页
The rare radioactive-isotope(RI)ring is an isochronous storage ring for deriving the masses of extremely short-lived rare RIs.Since the successful commissioning experiment in 2015,the time of flight mass measurement t... The rare radioactive-isotope(RI)ring is an isochronous storage ring for deriving the masses of extremely short-lived rare RIs.Since the successful commissioning experiment in 2015,the time of flight mass measurement technique has been established through test experiments using unstable nuclei with well-known masses.The experiments for unknown masses were started in 2018.While conducting experiments,we continue to develop equipment to further improve the efficiency and precision of mass measurements.The upgraded kicker system can generate a magnetic field with an extractable duration equivalent to the revolution time of the ring.This is essential for extracting extremely rare events as well as shortening the measurement time compared with that in the initial experiments.New steering magnets make it possible to eliminate an uncertain vertical beam deviation that occurs upstream.As a result,we confirm that the extraction yield is increased.A new resonant Schottky pick-up is able to detect single particles in timeframes on the order of milliseconds.It will be useful not only for beam diagnostics but also for lifetime measurement experiments of extremely short-lived rare RIs planned as a future application. 展开更多
关键词 steering magnet kicker system Schottky pick-up isochronous storage ring
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Potential to identify neutrino mass ordering with reactor antineutrinos at JUNO
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作者 Angel Abusleme Thomas Adam +628 位作者 Shakeel Ahmad Rizwan Ahmed Sebastiano Aiello Muhammad Akram Abid Aleem Fengpeng An Qi An Giuseppe Andronico Nikolay Anfimov Vito Antonelli Tatiana Antoshkina Burin Asavapibhop João Pedro Athayde Marcondes de André Didier Auguste Weidong Bai Nikita Balashov Wander Baldini Andrea Barresi Davide Basilico Eric Baussan Marco Bellato Marco Beretta Antonio Bergnoli Daniel Bick Lukas Bieger Svetlana Biktemerova Thilo Birkenfeld Iwan Morton-Blake David Blum Simon Blyth Anastasia Bolshakova Mathieu Bongrand Clément Bordereau Dominique Breton Augusto Brigatti Riccardo Brugnera Riccardo Bruno Antonio Budano Jose Busto Anatael Cabrera Barbara Caccianiga Hao Cai Xiao Cai Yanke Cai Zhiyan Cai Stéphane Callier Antonio Cammi Agustin Campeny Chuanya Cao Guofu Cao Jun Cao Rossella Caruso Cédric Cerna Vanessa Cerrone Chi Chan Jinfan Chang Yun Chang Auttakit Chatrabhuti Chao Chen Guoming Chen Pingping Chen Shaomin Chen Yixue Chen Yu Chen Zhangming Chen Zhiyuan Chen Zikang Chen Jie Cheng Yaping Cheng Yu Chin Cheng Alexander Chepurnov Alexey Chetverikov Davide Chiesa Pietro Chimenti Yen-Ting Chin Ziliang Chu Artem Chukanov Gérard Claverie Catia Clementi Barbara Clerbaux Marta Colomer Molla Selma Conforti DiLorenzo Alberto Coppi Daniele Corti Simon Csakli Flavio Dal Corso Olivia Dalager Jaydeep Datta Christophe De La Taille Zhi Deng Ziyan Deng Xiaoyu Ding Xuefeng Ding Yayun Ding Bayu Dirgantara Carsten Dittrich Sergey Dmitrievsky Tadeas Dohnal Dmitry Dolzhikov Georgy Donchenko Jianmeng Dong Evgeny Doroshkevich Wei Dou Marcos Dracos Frédéric Druillole Ran Du Shuxian Du Katherine Dugas Stefano Dusini Hongyue Duyang Jessica Eck Timo Enqvist Andrea Fabbri Ulrike Fahrendholz Lei Fan Jian Fang Wenxing Fang Marco Fargetta Dmitry Fedoseev Zhengyong Fei Li-Cheng Feng Qichun Feng Federico Ferraro Amélie Fournier Haonan Gan Feng Gao Alberto Garfagnini Arsenii Gavrikov Marco Giammarchi Nunzio Giudice Maxim Gonchar Guanghua Gong Hui Gong Yuri Gornushkin Alexandre Göttela Marco Grassi Maxim Gromov Vasily Gromov Minghao Gu Xiaofei Gu Yu Gu Mengyun Guan Yuduo Guan Nunzio Guardone Cong Guo Wanlei Guo Xinheng Guo Caren Hagner Ran Han Yang Han Miao He Wei He Tobias Heinz Patrick Hellmuth Yuekun Heng Rafael Herrera YuenKeung Hor Shaojing Hou Yee Hsiung Bei-Zhen Hu Hang Hu Jianrun Hu Jun Hu Shouyang Hu Tao Hu Yuxiang Hu Zhuojun Hu Guihong Huang Hanxiong Huang Jinhao Huang Junting Huang Kaixuan Huang Wenhao Huang Xin Huang Xingtao Huang Yongbo Huang Jiaqi Hui Lei Huo Wenju Huo Cédric Huss Safeer Hussain Leonard Imbert Ara Ioannisian Roberto Isocrate Arshak Jafar Beatrice Jelmini Ignacio Jeria Xiaolu Ji Huihui Jia Junji Jia Siyu Jian Cailian Jiang Di DiJiang Wei Jiang Xiaoshan Jiang Xiaoping Jing Cécile Jollet Philipp Kampmann Li Kang Rebin Karaparambil Narine Kazarian Khan Ali Amina Khatun Khanchai Khosonthongkee Denis Korablev Konstantin Kouzakov Alexey Krasnoperov Sergey Kuleshov Nikolay Kutovskiy Loïc Labit Tobias Lachenmaier Cecilia Landini Sébastien Leblanc Victor Lebrin Frederic Lefevre Ruiting Lei Rupert Leitner Jason Leung Demin Li Fei Li Fule Li Gaosong Li Jiajun Li Mengzhao Li Min Li Nan Li Qingjiang Li Ruhui Li Rui Li Shanfeng Li Tao Li Teng Li Weidong Li Weiguo Li Xiaomei Li Xiaonan Li Xinglong Li Yi Li Yichen Li Yufeng Li Zhaohan Li Zhibing Li Ziyuan Li Zonghai Li Hao Liang Hao Liang Jiajun Liao Ayut Limphirat Guey-Lin Lin Shengxin Lin Tao Lin Jiajie Ling Xin Ling Ivano Lippi Caimei Liu Fang Liu Fengcheng Liu Haidong Liu Haotian Liu Hongbang Liu Hongjuan Liu Hongtao Liu Hui Liu Jianglai Liu Jiaxi Liu Jinchang Liu Min Liu Qian Liu Qin Liu Runxuan Liu Shenghui Liu Shubin Liu Shulin Liu Xiaowei Liu Xiwen Liu Xuewei Liu Yankai Liu Zhen Liu Alexey Lokhov Paolo Lombardi Claudio Lombardo Kai Loo Chuan Lu Haoqi Lu Jingbin Lu Junguang Lu Peizhi Lu Shuxiang Lu Bayarto Lubsandorzhiev Sultim Lubsandorzhiev Livia Ludhova Arslan Lukanov Daibin Luo Fengjiao Luo Guang Luo Jianyi Luo Shu Luo Wuming Luo Xiaojie Luo Vladimir Lyashuk Bangzheng Ma Bing Ma Qiumei Ma Si Ma Xiaoyan Ma Xubo Ma Jihane Maalmi Marco Magoni Jingyu Mai Yury Malyshkin Roberto Carlos Mandujano Fabio Mantovani Xin Mao Yajun Mao Stefano M.Mari Filippo Marini Agnese Martini Matthias Mayer Davit Mayilyan Ints Mednieks Yue Meng Anita Meraviglia Anselmo Meregaglia Emanuela Meroni David Meyhöfer Lino Miramonti Nikhil Mohan Michele Montuschi Axel Müller Massimiliano Nastasi Dmitry V.Naumov Elena Naumova Diana Navas-Nicolas Igor Nemchenok Minh Thuan Nguyen Thi Alexey Nikolaev Feipeng Ning Zhe Ning Hiroshi Nunokawa Lothar Oberauer Juan Pedro Ochoa-Ricoux Alexander Olshevskiy Domizia Orestano Fausto Ortica Rainer Othegraven Alessandro Paoloni Sergio Parmeggiano Yatian Pei Luca Pelicci Anguo Peng Haiping Peng Yu Peng Zhaoyuan Peng Frédéric Perrot Pierre-Alexandre Petitjean Fabrizio Petrucci Oliver Pilarczyk Luis Felipe Piñeres Rico Artyom Popov Pascal Poussot Ezio Previtali Fazhi Qi Ming Qi Xiaohui Qi Sen Qian Xiaohui Qian Zhen Qian Hao Qiao Zhonghua Qin Shoukang Qiu Manhao Qu Zhenning Qu Gioacchino Ranucci Reem Rasheed Alessandra Re Abdel Rebii Mariia Redchuk Bin Ren Jie Ren Barbara Ricci Komkrit Rientong Mariam Rifai Mathieu Roche Narongkiat Rodphai Aldo Romani Bedřich Roskovec Xichao Ruan Arseniy Rybnikov Andrey Sadovsky Paolo Saggese Deshan Sandanayake Anut Sangka Giuseppe Sava Utane Sawangwit Michaela Schever Cédric Schwab Konstantin Schweizer Alexandr Selyunin Andrea Serafini Mariangela Settimo Vladislav Sharov Arina Shaydurova Jingyan Shi Yanan Shi Vitaly Shutov Andrey Sidorenkov FedorŠimkovic Apeksha Singhal Chiara Sirignano Jaruchit Siripak Monica Sisti Mikhail Smirnov Oleg Smirnov Thiago Sogo-Bezerra Sergey Sokolov Julanan Songwadhana Boonrucksar Soonthornthum Albert Sotnikov OndřejŠrámek Warintorn Sreethawong Achim Stahl Luca Stanco Konstantin Stankevich Hans Steiger Jochen Steinmann Tobias Sterr Matthias Raphael Stock Virginia Strati Alexander Studenikin Aoqi Su Jun Su Shifeng Sun Xilei Sun Yongjie Sun Yongzhao Sun Zhengyang Sun Narumon Suwonjandee Michal Szelezniak Akira Takenaka Jian Tang Qiang Tang Quan Tang Xiao Tang Vidhya Thara Hariharan Eric Theisen Alexander Tietzsch Igor Tkachev Tomas Tmej Marco Danilo Claudio Torri Francesco Tortorici Konstantin Treskov Andrea Triossi Riccardo Triozzi Wladyslaw Trzaska Yu-Chen Tung Cristina Tuve Nikita Ushakov Vadim Vedin Carlo Venettacci Giuseppe Verde Maxim Vialkov Benoit Viaud Cornelius Moritz Vollbrecht Katharinavon Sturm Vit Vorobel Dmitriy Voronin Lucia Votano Pablo Walker Caishen Wang Chung-Hsiang Wang En Wang Guoli Wang Jian Wang Jun Wang Li Wang Lu Wang Meng Wang Meng Wang Ruiguang Wang Siguang Wang Wei Wang Wenshuai Wang Xi Wang Xiangyue Wang Yangfu Wang Yaoguang Wang Yi Wang Yi Wang Yifang Wang Yuanqing Wang Yuyi Wang Zhe Wang Zheng Wang Zhimin Wang Apimook Watcharangkool Wei Wei Wei Wei Wenlu Wei Yadong Wei Yuehuan Wei Kaile Wen Liangjian Wen Jun Weng Christopher Wiebusch Rosmarie Wirth Bjoern Wonsak Diru Wu Qun Wu Yiyang Wu Zhi Wu Michael Wurm Jacques Wurtz Christian Wysotzki Yufei Xi Dongmei Xia Fei Xiao Xiang Xiao Xiaochuan Xie Yuguang Xie Zhangquan Xie Zhao Xin Zhizhong Xing Benda Xu Cheng Xu Donglian Xu Fanrong Xu Hangkun Xu Jilei Xu Jing Xu Meihang Xu Xunjie Xu Yin Xu Yu Xu Baojun Yan Qiyu Yan Taylor Yan Xiongbo Yan Yupeng Yan Changgen Yang Chengfeng Yang Jie Yang Lei Yang Xiaoyu Yang Yifan Yang Yifan Yang Haifeng Yao Jiaxuan Ye Mei Ye Ziping Ye Frédéric Yermia Zhengyun You Boxiang Yu Chiye Yu Chunxu Yu Guojun Yu Hongzhao Yu Miao Yu Xianghui Yu Zeyuan Yu Zezhong Yu Cenxi Yuan Chengzhuo Yuan Ying Yuan Zhenxiong Yuan Baobiao Yue Noman ZafarV italii Zavadskyi Fanrui Zeng Shan Zeng Tingxuan Zeng Yuda Zeng Liang Zhan Aiqiang Zhang Bin Zhang Binting Zhang Feiyang Zhang Haosen Zhang Honghao Zhang Jialiang Zhang Jiawen Zhang Jie Zhang Jingbo Zhang Jinnan Zhang Han Zhang Lei Zhang Mohan Zhang Peng Zhang Ping Zhang Qingmin Zhang Shiqi Zhang Shu Zhang Shuihan Zhang Siyuan Zhang Tao Zhang Xiaomei Zhang Xin Zhang Xuantong Zhang Yinhong Zhang Yiyu Zhang Yongpeng Zhang Yu Zhang Yuanyuan Zhang Yumei Zhang Zhenyu Zhang Zhijian Zhang Jie Zhao Rong Zhao Runze Zhao Shujun Zhao Dongqin Zheng Hua Zheng Yangheng Zheng Weirong Zhong Jing Zhou Li Zhou Nan Zhou Shun Zhou Tong Zhou Xiang Zhou Jingsen Zhu Kangfu Zhu Kejun Zhu Zhihang Zhu Bo Zhuang Honglin Zhuang Liang Zong Jiaheng Zou Jan Züfle The JUNO Collaboration 《Chinese Physics C》 2025年第3期37-63,共27页
The Jiangmen Underground Neutrino Observatory(JUNO)is a multi-purpose neutrino experiment under construction in South China.This paper presents an updated estimate of JUNO’s sensitivity to neutrino mass ordering usin... The Jiangmen Underground Neutrino Observatory(JUNO)is a multi-purpose neutrino experiment under construction in South China.This paper presents an updated estimate of JUNO’s sensitivity to neutrino mass ordering using the reactor antineutrinos emitted from eight nuclear reactor cores in the Taishan and Yangjiang nuclear power plants.This measurement is planned by studying the fine interference pattern caused by quasi-vacuum oscillations in the oscillated antineutrino spectrum at a baseline of 52.5 km and is completely independent of the CP violating phase and neutrino mixing angleθ_(23).The sensitivity is obtained through a joint analysis of JUNO and Taishan Antineutrino Observatory(TAO)detectors utilizing the best available knowledge to date about the location and overburden of the JUNO experimental site,local and global nuclear reactors,JUNO and TAO detector responses,expected event rates and spectra of signals and backgrounds,and systematic uncertainties of analysis inputs.We find that a 3σmedian sensitivity to reject the wrong mass ordering hypothesis can be reached with an exposure of about 6.5 years×26.6 GW thermal power. 展开更多
关键词 JUNO NEUTRINO neutrino mass ordering
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Prediction of energy resolution in the JUNO experiment
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作者 Angel Abusleme Thomas Adam +651 位作者 Kai Adamowicz Shakeel Ahmad Rizwan Ahmed Sebastiano Aiello Fengpeng An Qi An Giuseppe Andronico Nikolay Anfimov Vito Antonelli Tatiana Antoshkina Joao Pedro Athayde Marcondes de André Didier Auguste Weidong Bai Nikita Balashov Wander Baldini Andrea Barresi Davide Basilico Eric Baussan Marco Bellato Marco Beretta Antonio Bergnoli Daniel Bick Lukas Bieger Svetlana Biktemerova Thilo Birkenfeld Iwan Blake David Blum Simon Blyth Anastasia Bolshakova Mathieu Bongrand Clément Bordereau Dominique Breton Augusto Brigatti Riccardo Brugnera Riccardo Bruno Antonio Budano Jose Busto Anatael Cabrera Barbara Caccianiga Hao Cai Xiao Cai Yanke Cai Zhiyan Cai Stéphane Callier Steven Calvez Antonio Cammi Agustin Campeny Chuanya Cao Guofu Cao Jun Cao Rossella Caruso Cédric Cerna Vanessa Cerrone Jinfan Chang Yun Chang Auttakit Chatrabhuti Chao Chen Guoming Chen Pingping Chen Shaomin Chen Xin Chen Yiming Chen Yixue Chen Yu Chen Zelin Chen Zhangming Chen Zhiyuan Chen Zikang Chen Jie Cheng Yaping Cheng YuChin Cheng Alexander Chepurnov Alexey Chetverikov Davide Chiesa Pietro Chimenti Yen-Ting Chin Po-Lin Chou Ziliang Chu Artem Chukanov Gérard Claverie Catia Clementi Barbara Clerbaux Marta Colomer Molla Selma Conforti Di Lorenzo Alberto Coppi Daniele Corti Simon Csakli Chenyang Cui Flavio Dal Corso Olivia Dalager Jaydeep Datta Christophe De La Taille Zhi Deng Ziyan Deng Xiaoyu Ding Xuefeng Ding Yayun Ding Bayu Dirgantara Carsten Dittrich Sergey Dmitrievsky Tadeas Dohnal Dmitry Dolzhikov Georgy Donchenko Jianmeng Dong Evgeny Doroshkevich Wei Dou Marcos Dracos Frédéric Druillole Ran Du Shuxian Du Katherine Dugas Stefano Dusini Hongyue Duyang Jessica Eck Timo Enqvist Andrea Fabbri Ulrike Fahrendholz Lei Fan Jian Fang Wenxing Fang Dmitry Fedoseev Li-Cheng Feng Qichun Feng Federico Ferraro Amélie Fournier Fritsch Fritsch Haonan Gan Feng Gao Feng Gao Alberto Garfagnini Arsenii Gavrikov Marco Giammarchi Nunzio Giudice Maxim Gonchar Guanghua Gong Hui Gong Yuri Gornushkin Marco Grassi Maxim Gromov Vasily Gromov Minghao Gu Xiaofei Gu Yu Gu Mengyun Guan Yuduo Guan Nunzio Guardone Rosa Maria Guizzetti Cong Guo Wanlei Guo Caren Hagner Hechong Han Ran Han Yang Han Miao He Wei He Xinhai He Tobias Heinz Patrick Hellmuth Yuekun Heng Rafael Herrera YuenKeung Hor Shaojing Hou Yee Hsiung Bei-Zhen Hu Hang Hu Jun Hu Peng Hu Shouyang Hu Tao Hu Yuxiang Hu Zhuojun Hu Guihong Huang Hanxiong Huang Jinhao Huang Junting Huang Kaixuan Huang Shengheng Huang Wenhao Huang Xin Huang Xingtao Huang Yongbo Huang Jiaqi Hui Lei Huo Wenju Huo Cédric Huss Safeer Hussain Leonard Imbert Ara Ioannisian Roberto Isocrate Arshak Jafar Beatrice Jelmini Ignacio Jeria Xiaolu Ji Huihui Jia Junji Jia Siyu Jian Cailian Jiang Di Jiang Wei Jiang Xiaoshan Jiang Xiaozhao Jiang Yixuan Jiang Xiaoping Jing Cécile Jollet Li Kang Rebin Karaparabil Narine Kazarian Ali Khan Amina Khatun Khanchai Khosonthongkee Denis Korablev Konstantin Kouzakov Alexey Krasnoperov Sergey Kuleshov Sindhujha Kumaran Nikolay Kutovskiy Loic Labit Tobias Lachenmaier Cecilia Landini Sébastien Leblanc Frederic Lefevre Ruiting Lei Rupert Leitner Jason Leung Demin Li Fei Li Fule Li Gaosong Li Hongjian Li Jiajun Li Min Li Nan Li Qingjiang Li Ruhui Li Rui Li Shanfeng Li Shuo Li Tao Li Teng Li Weidong Li Weiguo Li Xiaomei Li Xiaonan Li Xinglong Li Yi Li Yichen Li Yufeng Li Zhaohan Li Zhibing Li Ziyuan Li Zonghai Li Hao Liang Hao Liang Jiajun Liao Yilin Liao Yuzhong Liao Ayut Limphirat Guey-Lin Lin Shengxin Lin Tao Lin Jiajie Ling Xin Ling Ivano Lippi Caimei Liu Fang Liu Fengcheng Liu Haidong Liu Haotian Liu Hongbang Liu Hongjuan Liu Hongtao Liu Hongyang Liu Jianglai Liu Jiaxi Liu Jinchang Liu Min Liu Qian Liu Qin Liu Runxuan Liu Shenghui Liu Shubin Liu Shulin Liu Xiaowei Liu Xiwen Liu Xuewei Liu Yankai Liu Zhen Liu Lorenzo Loi Alexey Lokhov Paolo Lombardi Claudio Lombardo Kai Loo Chuan Lu Haoqi Lu Jingbin Lu Junguang Lu Meishu Lu Peizhi Lu Shuxiang Lu Bayarto Lubsandorzhiev Sultim Lubsandorzhiev Livia Ludhova Arslan Lukanov Fengjiao Luo Guang Luo Jianyi Luo Shu Luo Wuming Luo Xiaojie Luo Vladimir Lyashuk Bangzheng Ma Bing Ma Qiumei Ma Si Ma Xiaoyan Ma Xubo Ma Jihane Maalmi Jingyu Mai Marco Malabarba Yury Malyshkin Roberto Carlos Mandujano Fabio Mantovani Xin Mao Yajun Mao Stefano M.Mari Filippo Marini Agnese Martini Matthias Mayer Davit Mayilyan Ints Mednieks Yue Meng Anita Meraviglia Anselmo Meregaglia Emanuela Meroni Lino Miramonti Nikhil Mohan Michele Montuschi Axel Müller Massimiliano Nastasi Dmitry V.Naumov Elena Naumova Diana Navas-Nicolas Igor Nemchenok Minh Thuan Nguyen Thi Alexey Nikolaev Feipeng Ning Zhe Ning Hiroshi Nunokawa Lothar Oberauer Juan Pedro Ochoa-Ricoux Alexander Olshevskiy Domizia Orestano Fausto Ortica Rainer Othegraven Alessandro Paoloni George Parker Sergio Parmeggiano Achilleas Patsias Yatian Pei Luca Pelicci Anguo Peng Haiping Peng Yu Peng Zhaoyuan Peng Elisa Percalli Willy Perrin Frédéric Perrot Pierre-Alexandre Petitjean Fabrizio Petrucci Oliver Pilarczyk Luis Felipe Pineres Rico Artyom Popov Pascal PoussotE zio Previtali Fazhi Qi Ming Qi Xiaohui Qi Sen Qian Xiaohui Qian Zhen Qian Hao Qiao Zhonghua Qin Shoukang Qiu Manhao Qu Zhenning Qu Gioacchino Ranucci Reem Rasheed Alessandra Re Abdel Rebii Mariia Redchuk Gioele Reina Bin Ren Jie Ren Yuhan Ren Barbara Ricci Komkrit Rientong Mariam Rifai Mathieu Roche Narongkiat Rodphai Aldo Romani Bedrich Roskovec Xichao Ruan Arseniy Rybnikov Andrey Sadovsky Paolo Saggese Deshan Sandanayake Anut Sangka Giuseppe Sava Utane Sawangwit Michaela Schever Cédric Schwab Konstantin Schweizer Alexandr Selyunin Andrea Serafini Mariangela Settimo Junyu Shao Vladislav Sharov Hexi Shi Jingyan Shi Yanan Shi Vitaly Shutov Andrey Sidorenkov Fedor Simkovic Apeksha Singhal Chiara Sirignano Jaruchit Siripak Monica Sisti Mikhail Smirnov Oleg Smirnov Sergey Sokolov Julanan Songwadhana Boonrucksar Soonthornthum Albert Sotnikov Warintorn Sreethawong Achim Stahl Luca Stanco Konstantin Stankevich Hans Steiger Jochen Steinmann Tobias Sterr Matthias Raphael Stock Virginia Strati Michail Strizh Alexander Studenikin Aoqi SuJun Su Jun Su Shifeng Sun Xilei Sun Yongjie Sun Yongzhao Sun Zhengyang Sun Narumon Suwonjandee Akira Takenaka Xiaohan Tan Jian Tang Jingzhe Tang Qiang Tang Quan Tang Xiao Tang Vidhya Thara Hariharan Alexander Tietzsch Igor Tkachev Tomas Tmej Marco Danilo Claudio Torri Andrea Triossi Riccardo Triozzi Wladyslaw Trzaska Yu-Chen Tung Cristina Tuve Nikita Ushakov Vadim Vedin Carlo Venettacci Giuseppe Verde Maxim Vialkov Benoit Viaud Cornelius Moritz Vollbrecht Katharina von Sturm Vit Vorobel Dmitriy Voronin Lucia Votano Pablo Walker Caishen Wang Chung-Hsiang Wang En Wang Guoli Wang Jian Wang Jun Wang Li Wang Lu Wang Meng Wang Meng Wang Mingyuan Wang Ruiguang Wang Sibo Wang Siguang Wang Wei Wang Wenshuai Wang Xi Wang Xiangyue Wang Yangfu Wang Yaoguang Wang Yi Wang Yi Wang Yifang Wang Yuanqing Wang Yuyi Wang Zhe Wang Zheng Wang Zhimin Wang Apimook Watcharangkool Wei Wei Wei Wei Wenlu Wei Yadong Wei Yuehuan Wei Kaile Wen Liangjian Wen Jun Weng Christopher Wiebusch Rosmarie Wirth Chengxin Wu Diru Wu Qun Wu Yinhui Wu Yiyang Wu Zhi Wu Michael Wurm Jacques Wurtz Christian Wysotzki Yufei Xi Dongmei Xia Shishen Xian Fei Xiao Xiang Xiao Xiaochuan Xie Yijun Xie Yuguang Xie Zhao Xin Zhizhong Xing Benda Xu Cheng Xu Donglian Xu Fanrong Xu Hangkun Xu Jiayang Xu Jilei Xu Jing Xu Jinghuan Xu Meihang Xu Xunjie Xu Yin Xu Yu Xu Baojun Yan Qiyu Yan Taylor Yan Xiongbo Yan Yupeng Yan Changgen Yang Chengfeng Yang Fengfan Yang Jie Yang Lei Yang Pengfei Yang Xiaoyu Yang Yifan Yang Yixiang Yang Zekun Yang Haifeng Yao Jiaxuan Ye Mei Ye Ziping Ye Frédéric Yermia Zhengyun You Boxiang Yu Chiye Yu Chunxu Yu Guojun Yu Hongzhao Yu Miao Yu Xianghui Yu Zeyuan Yu Zezhong Yu Cenxi Yuan Chengzhuo Yuan Ying Yuan Zhenxiong Yuan Baobiao Yue Noman Zafar Kirill Zamogilnyi Vitalii Zavadskyi Fanrui Zeng Shan Zeng Tingxuan Zeng Yuda Zeng Liang Zhan Yonghua Zhan Aiqiang Zhang Bin Zhang Binting Zhang Feiyang Zhang Hangchang Zhang Haosen Zhang Honghao Zhang Jialiang Zhang Jiawen Zhang Jie Zhang Jingbo Zhang Jinnan Zhang Junwei Zhang Lei Zhang Peng Zhang Ping Zhang Qingmin Zhang Shiqi Zhang Shu Zhang Shuihan Zhang Siyuan Zhang Tao Zhang Xiaomei Zhang Xin Zhang Xuantong Zhang Yinhong Zhang Yiyu Zhang Yongpeng Zhang Yu Zhang Yuanyuan Zhang Yumei Zhang Zhenyu Zhang Zhijian Zhang Jie Zhao Rong Zhao Runze Zhao Shujun Zhao Tianhao Zhao Hua Zheng Yangheng Zheng Jing Zhou Li Zhou Nan Zhou Shun Zhou Tong Zhou Xiang Zhou Jingsen Zhu Kangfu Zhu Kejun Zhu Zhihang Zhu Bo Zhuang Honglin Zhuang Liang Zong Jiaheng Zou Jan Züfle The JUNO Collaboration 《Chinese Physics C》 2025年第1期35-59,共25页
This paper presents an energy resolution study of the JUNO experiment,incorporating the latest knowledge acquired during the detector construction phase.The determination of neutrino mass ordering in JUNO requires an ... This paper presents an energy resolution study of the JUNO experiment,incorporating the latest knowledge acquired during the detector construction phase.The determination of neutrino mass ordering in JUNO requires an exceptional energy resolution better than 3% at 1 MeV.To achieve this ambitious goal,significant efforts have been undertaken in the design and production of the key components of the JUNO detector.Various factors affecting the detection of inverse beta decay signals have an impact on the energy resolution,extending beyond the statistical fluctuations of the detected number of photons,such as the properties of the liquid scintillator,performance of photomultiplier tubes,and the energy reconstruction algorithm.To account for these effects,a full JUNO simulation and reconstruction approach is employed.This enables the modeling of all relevant effects and the evaluation of associated inputs to accurately estimate the energy resolution.The results of this study reveal an energy resolution of 2.95% at 1 Mev.Furthermore,this study assesses the contribution of major effects to the overall energy resolution budget.This analysis serves as a reference for interpreting future measurements of energy resolution during JUNO data collection.Moreover,it provides a guideline for comprehending the energy resolution characteristics of liquid scintillator-based detectors. 展开更多
关键词 energy resolution liquid scintillator detector JUNO SIMULATION RECONSTRUCTION
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The NUBASE2020 evaluation of nuclear physics properties 被引量:37
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作者 F.G.Kondev M.Wang +2 位作者 W.J.Huang S.Naimi G.Audi 《Chinese Physics C》 SCIE CAS CSCD 2021年第3期1-180,共180页
The NUBASE2020 evaluation contains the recommended values of the main nuclear physics properties for all nuclei in their ground and excited,isomeric(T1/2≥100 ns)states.It encompasses all experimental data published i... The NUBASE2020 evaluation contains the recommended values of the main nuclear physics properties for all nuclei in their ground and excited,isomeric(T1/2≥100 ns)states.It encompasses all experimental data published in primary(journal articles)and secondary(mainly laboratory reports and conference proceedings)references,together with the corresponding bibliographical information.In cases where no experimental data were available for a particular nuclide,trends in the behavior of specific properties in neighboring nuclei were examined and estimated values are proposed.Evaluation procedures and policies that were used during the development of this evaluated nuclear data library are presented,together with a detailed table of recommended values and their uncertainties. 展开更多
关键词 NUBASE2020 evaluation nuclear properties atomic masses ISOMERS excitation energy of isomers spin and parity HALF-LIFE year of discovery decay modes
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The Ame2020 atomic mass evaluation(II).Tables,graphs and references 被引量:42
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作者 Meng Wang W.J.Huang +2 位作者 F.G.Kondev G.Audi S.Naimi 《Chinese Physics C》 SCIE CAS CSCD 2021年第3期523-1034,共512页
This is the second part of the new evaluation of atomic masses,Ame2020.Using least-squares adjustments to all evaluated and accepted experimental data,described in Part I,we derived tables with numerical values and gr... This is the second part of the new evaluation of atomic masses,Ame2020.Using least-squares adjustments to all evaluated and accepted experimental data,described in Part I,we derived tables with numerical values and graphs which supersede those given in Ame2016.The first table presents the recommended atomic mass values and their uncertainties.It is followed by a table of the influences of data on primary nuclides,a table of various reaction and decay energies,and finally,a series of graphs of separation and decay energies.The last section of this paper provides all input data references that were used in the Ame2020 and the Nubase2020 evaluations. 展开更多
关键词 atomic mass evaluation atomic mass table separation and reaction energies trends from the mass surface
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Isomeric pair 95m,g Nb in the photonuclear reactions on natMo at the bremsstrahlung end-point energy of 38–93 MeV 被引量:1
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作者 I.S.Timchenko O.S.Deiev +5 位作者 S.M.Olejnik S.M.Potin V.A.Kushnir V.V.Mytrochenko S.A.Perezhogin V.A.Bocharov 《Chinese Physics C》 SCIE CAS CSCD 2023年第12期64-72,共9页
The^(nat)Mo(γ,xnp)^(95m,g)Nb photonuclear reaction was studied using the electron beam from the NSC KIPT linear accelerator LUE-40.The experiment was performed using the activation and off-lineγ-ray spectrometric te... The^(nat)Mo(γ,xnp)^(95m,g)Nb photonuclear reaction was studied using the electron beam from the NSC KIPT linear accelerator LUE-40.The experiment was performed using the activation and off-lineγ-ray spectrometric technique.The experimental isomeric yield ratio(IR)was determined for the reaction products^(95m,g)Nb at the bremsstrahlung end-point energy E_(γmax)range of 38-93 MeV.The obtained values of IR are in satisfactory agreement with the results of other studies and extend the range of previously known data.The theoretical values of the yields Y_(m,g)(E_(γmax))and the IR for the isomeric pair^(95m,g)Nb from the^(nat)Mo(γ,xnp)reaction were calculated using the partial cross-sectionsσ(E)from the TALYS1.95 code for six different level density models.For the investigated range of E_(γmax),the theoretical dependence of IR on energy was confirmed-the IR smoothly increases with increasing energy.The comparison showed a noticeable difference(more than 3.85 times)in the experimental IR relative to all theoretical estimates. 展开更多
关键词 photonuclear reactions natMo isomeric pair 95m gNb isomeric yield ratio reaction yield bremsstrahlung end-point energy of 38–93 MeV activation and off-lineγ-ray spectrometric technique TALYS1.95 level density model GEANT4.9.2.
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Robustness of chiral symmetry in atomic nuclei with reflectionasymmetric shapes
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作者 Costel Marian Petrache 《Science Bulletin》 SCIE EI CSCD 2020年第23期1956-1957,共2页
Nearly degenerate quantum states arise from fundamental symmetries, which are often broken in finite many-body systems like atomic nuclei. Chirality can be static, like in molecules composed of more than four atoms, o... Nearly degenerate quantum states arise from fundamental symmetries, which are often broken in finite many-body systems like atomic nuclei. Chirality can be static, like in molecules composed of more than four atoms, or dynamic, like in particle physics distinguishing between parallel and antiparallel orientation of the spin with respect to the momentum of massless fermions. 展开更多
关键词 手征对称性 MOMENTUM DEGENERATE
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