Shear band evolution and acoustic emission characteristics of sandstone containing non-persistent flaws 认领 引用 被引量：1

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作者 Shuting Miao Peng-Zhi Pan +1 位作者 Chuanqing Zhang Lei Huo 《Journal of Rock Mechanics and Geotechnical Engineering》 SCIE CSCD 2024年第2期497-513,共17页

Direct shear tests were conducted on sandstone specimens under different constant normal stresses to study the coalescence of cracks between non-persistent flaws and the shear sliding characteristics of the shear-form... Direct shear tests were conducted on sandstone specimens under different constant normal stresses to study the coalescence of cracks between non-persistent flaws and the shear sliding characteristics of the shear-formed fault.Digital image correlation and acoustic emission(AE)techniques were used to monitor the evolution of shear bands at the rock bridge area and microcracking behaviors.The experimental results revealed that the shear stresses corresponding to the peak and sub-peak in the stressdisplacement curve are significantly affected by the normal stress.Strain localization bands emerged at both the tip of joints and the rock bridge,and their extension and interaction near the peak stress caused a surge in the AE hit rate and a significant decrease in the AE b value.Short and curvilinear strain bands were detected at low normal stress,while high normal stress generally led to more microcracking events and longer coplanar cracks at the rock bridge area.Furthermore,an increase in normal stress resulted in a higher AE count rate and more energetic AE events during friction sliding along the shearformed fault.It was observed that the elastic energy released during the crack coalescence at the prepeak stage was much greater than that released during friction sliding at the post-peak stage.More than 75%of AE events were located in the low-frequency band(0e100 kHz),and this proportion continued to rise with increasing normal stress.Moreover,more AE events of low AF value and high RA value were observed in specimens subjected to high normal stress,indicating that greater normal stress led to more microcracks of shear nature. 展开更多

关键词 Shear band evolution Acoustic emission(AE) Crack coalescence Normal stress Shear sliding

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Tuning the intensity statistics of random speckle patterns 认领 引用

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作者 Fan Meng Yue Zhao +1 位作者 Yun-Zuo Zhang Lei Huo 《Chinese Physics B》 SCIE EI CAS CSCD 2019年第5期327-331,共5页

Speckle patterns are a fundamental tool in a variety of physical and optical applications. Here, we investigate a method of precisely tuning the intensity statistics of random speckle patterns into a desirable pattern... Speckle patterns are a fundamental tool in a variety of physical and optical applications. Here, we investigate a method of precisely tuning the intensity statistics of random speckle patterns into a desirable pattern that possesses the same spatial correlation length and similar statistics distribution. This tuning mechanism relies on the derivation of the transform function and transmission matrix, which achieves different contrasts while maintaining the same average value or energy level. The statistics properties of the generated speckle patterns are further investigated by analyzing the standard deviation under different fitting parameters. Precisely tuning the intensity statistics of random speckle patterns could be useful for both fundamental research and practical applications, such as microscopy, imaging, and optical manipulation. 展开更多

关键词 random speckle pattern intensity statistics local intensity transformation optical manipulation

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中国新诊断胶质母细胞瘤患者实际治疗方案与Stupp方案的一致性比较 认领 引用

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作者 Yu Wang Jianmin Zhang +27 位作者 Wenbin Li Taipeng Jiang Songtao Qi Zhongping Chen Jingbo Kang Lei Huo Yunjie Wang Qichuan Zhuge Guodong Gao Yuping Wu Hua Feng Gang Zhao Xiaopeng Yang Hui Zhao Yirong Wang Hui Yang Dezhi Kang Jun Su Liang Li Chuanlu Jiang Gang Li Yongming Qiu Weimin Wang Handong Wang Zaihua Xu Liwei Zhang Renzhi Wang 吴劲松 《癌症》 CAS 2022年第8期385-399,共15页

目的评估中国新诊断胶质母细胞瘤(glioblastoma multiforme,GBM)患者实际接受的治疗方案与指南推荐的Stupp方案的一致性。方法纳入202例新诊断GBM患者,评估实际接受的治疗方案与Stupp方案一致的患者比例,以及不符合Stupp方案的原因。结... 目的评估中国新诊断胶质母细胞瘤(glioblastoma multiforme,GBM)患者实际接受的治疗方案与指南推荐的Stupp方案的一致性。方法纳入202例新诊断GBM患者,评估实际接受的治疗方案与Stupp方案一致的患者比例,以及不符合Stupp方案的原因。结果研究发现,仅15.8%的GBM患者接受了与Stupp方案一致的治疗。治疗方案的不一致主要是由于同步放化疗阶段替莫唑胺剂量>75 mg/m²(58/120;48.3%)和治疗持续时间<42 d(84/120;70.0%),以及辅助治疗阶段替莫唑胺剂量<150 mg/m²(89/101;88.1%)。接受符合Stupp方案治疗的患者的中位总生存期(27.09 vs 18.21个月)和无进展生存期(14.27 vs 12.10个月)更长。结论需要提高中国GBM患者实际接受的治疗方案与Stupp方案的一致性。 展开更多

关键词 辅助化疗 一致性 胶质母细胞瘤 胶质瘤 Stupp方案 替莫唑胺

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Single-Choice Aided Marking System Research Based on Back Propagation Neural Network 认领 引用

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作者 Yunzuo Zhang Yi Li +3 位作者 Wei Guo Lei Huo Jiayu Zhang Kaina Guo 《Journal of Cyber Security》 2021年第1期45-54,共10页

In the field of educational examination,automatic marking technology plays an essential role in improving the efficiency of marking and liberating the labor force.At present,the implementation of the policy of expandi... In the field of educational examination,automatic marking technology plays an essential role in improving the efficiency of marking and liberating the labor force.At present,the implementation of the policy of expanding erolments has caused a serious decline in the teacher-student ratio in colleges and universities.The traditional marking system based on Optical Mark Reader technology can no longer meet the requirements of liberating the labor force of teachers in small and medium-sized examinations.With the development of image processing and artificial neural network technology,the recognition of handwritten character in the field of pattern recognition has attracted the attention of many researchers.In this paper,filtering and de-noise processing and binary processing are used as preprocessing methods for handwriting recognition.Extract the pixel feature of handwritten characters through digital image processing of handwritten character pictures,and then,get the feature vector from these feature fragments and use it as the description of the character.The extracted feature values are used to train the neural network to realize the recognition of handwritten English letters and numerical characters.Experimental results on Chars74K and MNIST data sets show that the recognition accuracy of some handwritten English letters and numerical characters can reach 90%and 99%,respectively. 展开更多

关键词 Image preprocessing BP neural network handwriting recognition marking system

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Upregulation of α-ENaC induces pancreatic β-cell dysfunction,ER stress,and SIRT2 degradation 认领 引用 被引量：1

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作者 Xue Zhang Dan Zhang +7 位作者 Lei Huo Xin Zhou Jia Zhang Min Li Dongming Su Peng Sun Fang Chen Xiubin Liang 《Journal of Biomedical Research》 CAS CSCD 2024年第3期241-255,共15页

Islet beta cells(β-cells)produce insulin in response to high blood glucose levels,which is essential for preserving glucose homeostasis.Voltage-gated ion channels inβ-cells,including Na+,K+,and Ca2+channels,aid in t... Islet beta cells(β-cells)produce insulin in response to high blood glucose levels,which is essential for preserving glucose homeostasis.Voltage-gated ion channels inβ-cells,including Na+,K+,and Ca2+channels,aid in the release of insulin.The epithelial sodium channel alpha subunit(α-ENaC),a voltage-independent sodium ion channel,is also expressed in human pancreatic endocrine cells.However,there is no reported study on the function of ENaC in theβ-cells.In the current study,we found thatα-ENaC was expressed in human pancreatic glandule and pancreatic isletβ-cells.In the pancreas of db/db mice and high-fat diet-induced mice,and in mouse isletβ-cells(MIN6 cells)treated with palmitate,α-ENaC expression was increased.Whenα-ENaC was overexpressed in MIN6 cells,insulin content and glucose-induced insulin secretion were significantly reduced.On the other hand,palmitate injured isletβ-cells and suppressed insulin synthesis and secretion,but increasedα-ENaC expression in MIN6 cells.However,α-ENaC knockout(Scnn1a−/−)in MIN6 cells attenuatedβ-cell disorder induced by palmitate.Furthermore,α-ENaC regulated the ubiquitylation and degradation of sirtuin 2 inβ-cells.α-ENaC also modulatedβ-cell function in correlation with the inositol-requiring enzyme 1 alpha/X-box binding protein 1(IRE1α/XBP1)and protein kinase RNA-like endoplasmic reticulum kinase/C/EBP homologous protein(PERK/CHOP)endoplasmic reticulum stress pathways.These results suggest thatα-ENaC may play a novel role in insulin synthesis and secretion in theβ-cells,and the upregulation ofα-ENaC promotes isletβ-cell dysfunction.In conclusion,α-ENaC may be a key regulator involved in isletβ-cell damage and a potential therapeutic target for type 2 diabetes mellitus. 展开更多

关键词 α-ENaC pancreaticβ-cells type 2 diabetes mellitus endoplasmic reticulum stress sirtuin 2

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Service Composition Instantiation Based on Cross-Modified Artificial Bee Colony Algorithm 认领 引用 被引量：1

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作者 Lei Huo Zhiliang Wang 《China Communications》 SCIE CSCD 2016年第10期233-244,共12页

Internet of things(IoT) imposes new challenges on service composition as it is difficult to manage a quick instantiation of a complex services from a growing number of dynamic candidate services. A cross-modified Arti... Internet of things(IoT) imposes new challenges on service composition as it is difficult to manage a quick instantiation of a complex services from a growing number of dynamic candidate services. A cross-modified Artificial Bee Colony Algorithm(CMABC) is proposed to achieve the optimal solution services in an acceptable time and high accuracy. Firstly, web service instantiation model was established. What is more, to overcome the problem of discrete and chaotic solution space, the global optimal solution was used to accelerate convergence rate by imitating the cross operation of Genetic algorithm(GA). The simulation experiment result shows that CMABC exhibited faster convergence speed and better convergence accuracy than some other intelligent optimization algorithms. 展开更多

关键词 optimization of service composition optimal service instantiation artificial bee colony algorithm swarm algorithm cross strategy

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Transmissivity of electromagnetic wave propagating in magnetized plasma sheath using variational method 认领 引用

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作者 Jianyi CHEN Chengxun YUAN +1 位作者 Xiudong SUN Lei HUO 《Plasma Science and Technology》 SCIE EI CAS CSCD 2019年第12期1-5,共5页

A variational method is introduced to analyze the transmissivity of an electromagnetic wave propagating in the magnetized plasma sheath. The plasma density is modeled by two parabolic inhomogeneous regions separated b... A variational method is introduced to analyze the transmissivity of an electromagnetic wave propagating in the magnetized plasma sheath. The plasma density is modeled by two parabolic inhomogeneous regions separated by one homogeneous region. The Lagrangian density of the system is constructed based on the fluid energy density and the electromagnetic energy density.The total variation of the Lagrangian density is derived. The fluid and electromagnetic fields are numerically solved by expansion in piecewise polynomial function space. We investigate the effect of an external magnetic field on the transmissivity of the electromagnetic wave. It is found that the transmissivity is increased when an external magnetic field is applied. The dependence of transmissivity on the collision frequency between the electrons and the neutral particles has also been studied. We also show that the external magnetic field causes a shift in the critical frequency of the plasma sheath. 展开更多

关键词 electromagnetic wave propagation variational method wave theory wave propagation plasma sheath

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影响颅内室管膜瘤患者生存和预后的相关因素分析 认领 引用 被引量：6

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作者 卞艺颖 陈伟鹏 +5 位作者 李战战 王颖 霍雷 魏瑞 申良方 洪继东 《中国肿瘤临床》 CAS CSCD 北大核心 2019年第3期138-144,共7页

目的:研究影响颅内室管膜瘤患者生存和预后的相关因素,为临床治疗提供理论依据。方法:回顾性分析2008年1月至2018年1月中南大学湘雅医院收治的颅内室管膜瘤患者276例,分析性别、年龄、肿瘤部位、肿瘤直径、手术切除程度、病理分级、Ki-6... 目的:研究影响颅内室管膜瘤患者生存和预后的相关因素,为临床治疗提供理论依据。方法:回顾性分析2008年1月至2018年1月中南大学湘雅医院收治的颅内室管膜瘤患者276例,分析性别、年龄、肿瘤部位、肿瘤直径、手术切除程度、病理分级、Ki-67指数、术后是否放疗、术后是否化疗对颅内室管膜瘤患者总生存时间和无进展生存时间的影响。结果:肿瘤部位、手术切除程度、术后是否放疗均能影响颅内室管膜瘤患者总生存时间和无进展生存时间(P<0.001),并且是影响总生存时间(P<0.001,P<0.001,P=0.002)和无进展生存时间(P<0.001,P<0.001,P<0.001)的独立因素;Ki-67指数是影响颅内室管膜瘤患者无进展生存的独立因素(P<0.001)。肿瘤位于幕上、Ki-67指数≥10%是提示预后不佳的独立危险因素(P<0.001),肿瘤全切、术后行放疗是保护因素(P<0.001,P=0.001)。结论:肿瘤部位、手术切除程度、Ki-67指数、术后是否放疗是响颅内室管膜瘤预后的独立因素,尽可能的肿瘤全切和术后放疗有助于延长患者的无进展生存时间和总生存时间。 展开更多

关键词 室管膜瘤 生存 预后 相关因素

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地应力条件下随钻四极子频散响应特征数值模拟及应用 认领 引用 被引量：3

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作者 黑创 雷豁 +3 位作者 罗明璋 李修权 张磊 付青青 《科学技术与工程》 北大核心 2019年第3期85-89,共5页

随钻四极子声波测井是目前随钻环境下测量地层横波速度的有效技术手段,地应力的存在会极大地影响地层横波速度的测量。为分析地应力对随钻四极子频散曲线的影响,通过微扰法建立随钻环境下地应力与频散曲线相速度改变量之间的关系,在此... 随钻四极子声波测井是目前随钻环境下测量地层横波速度的有效技术手段,地应力的存在会极大地影响地层横波速度的测量。为分析地应力对随钻四极子频散曲线的影响,通过微扰法建立随钻环境下地应力与频散曲线相速度改变量之间的关系,在此基础之上,研究了地应力作用下随钻四极子频散曲线的特征。数值模拟结果表明:与均匀地层相比,施加应力后随钻四极子频散曲线截止频率处的相速度明显增大;与裸眼井相比,由于钻挺的存在,随钻测井井孔附近的应力集中效应更为明显,但不会影响原状地层横波速度的测量。值得注意的是,地应力条件下随钻四极子频散曲线和以原状地层横波速度计算的均匀地层的频散曲线两者有较大差异,这可以作为判断地应力存在的一个依据。地应力条件下随钻四极子频散曲线的特征为随钻环境下地应力识别及反演提供了理论基础。 展开更多

关键词 随钻测井 多极子 地应力 频散曲线 应力集中

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井孔散射波数值模拟及提取方法 认领 引用 被引量：4

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作者 雷豁 黑创 +2 位作者 罗明璋 李修权 肖张波 《长江大学学报（自然科学版）》 2019年第12期15-19,78,共5页

井孔散射波携带了岩石的非均匀信息,可用于评价地下岩石的非均匀性,评价的前提是从全波数据中提取散射波.为了研究井孔弹性波散射效应及散射波的提取方法,建立了二维坐标系下的各向同性随机介质模型,利用有限差分数值模拟了偶极声波测... 井孔散射波携带了岩石的非均匀信息,可用于评价地下岩石的非均匀性,评价的前提是从全波数据中提取散射波.为了研究井孔弹性波散射效应及散射波的提取方法,建立了二维坐标系下的各向同性随机介质模型,利用有限差分数值模拟了偶极声波测井中的弹性非均匀性散射.模拟发现,偶极阵列波形产生了明显的尾波,其为散射波的一种体现形式,出现在直达波之后,主要来自于井外地层中的散射.在该基础之上,分析了偶极全波、直达波和尾波的频率-波数(F-K)域特征,并利用F-K滤波方法提取了尾波.将该方法应用于实际数据的散射波提取中,取得了较好的效果. 展开更多

关键词 散射效应 散射波 随机介质 有限差分 非均匀性 滤波

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基于YOLOv5s的CCTV排水管道缺陷识别方法研究 认领 引用 被引量：4

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作者 韩崔燕 周扬 +3 位作者 汪犁辉 雷豁 姚丹 梁卫清 《市政技术》 2024年第3期230-236,共7页

城市排水管道常出现堵塞、老化、腐蚀、破损等情况,严重影响城市的健康发展和市民的正常生活。通过分析当前排水管道缺陷识别方法的局限性,构建了基于YOLOv5s的排水管道缺陷识别模型,对10种常见的排水管道缺陷进行学习、训练和验证,通... 城市排水管道常出现堵塞、老化、腐蚀、破损等情况,严重影响城市的健康发展和市民的正常生活。通过分析当前排水管道缺陷识别方法的局限性,构建了基于YOLOv5s的排水管道缺陷识别模型,对10种常见的排水管道缺陷进行学习、训练和验证,通过数据收集、数据处理、模型训练和目标检测4个步骤,完成了排水管道缺陷的智能识别。实验结果表明,排水管道缺陷识别模型的多类别平均精确度达到了85.42%(其中错口、异物穿入、渗漏(附着型)和破裂4种缺陷识别的平均精确度分别达到了93.6%、91.7%、91.7%和91.3%),验证了该模型的有效性。另外,YOLOv5s模型相较于Faster R-CNN模型,多类别平均精确度更高,并且具有模型内存更小、检测速度更快的明显优势,大幅提升了模型的工程适用性。 展开更多

关键词 排水管道 CCTV 缺陷识别 YOLOv5s

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常州市排水基础设施安全运行监测平台建设与研究 认领 引用 被引量：8

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作者 陆文涛 陈波 +2 位作者 雷豁 邵慧星 秦一帆 《环境工程》 CAS CSCD 北大核心 2023年第11期25-33,共9页

排水系统是城市重要的基础设施之一,监测其运行状态意义重大。为解决排水系统数据管理、在线监测、业务管理、内涝预警等方面的问题,以常州市为研究对象,深入分析了排水系统现状及问题,并给出了解决方案。基于GIS、物联网、人工智能、... 排水系统是城市重要的基础设施之一,监测其运行状态意义重大。为解决排水系统数据管理、在线监测、业务管理、内涝预警等方面的问题,以常州市为研究对象,深入分析了排水系统现状及问题,并给出了解决方案。基于GIS、物联网、人工智能、数字孪生等技术,提出了排水基础设施安全运行监测技术架构,研发并建成排水基础设施安全运行监测平台。系统上线后,管网养护成本平均降低12%,污水全年低水位运行时间提升10%,一体化调度效率提升50%,实现了设施全生命周期管理、管网全方位监测、内涝高效预警与处置、厂网一体化调度,并有效提高了常州市排水基础设施数字化、智能化监管水平,可为同类城市相关工作提供参考。 展开更多

关键词 排水基础设施 监测平台 城市内涝预警 一体化调度

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Initial performance results of the JUNO detector 认领 引用

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作者 Angel Abusleme Thomas Adam +1137 位作者 Kai Adamowicz David Adey Shakeel Ahmad Rizwan Ahmed Timo Ahola Sebastiano Aiello Fengpeng An Guangpeng An Costas Andreopoulos Giuseppe Andronico João Pedro Athayde Marcondes de André Nikolay Anfimov Vito Antonelli Tatiana Antoshkina Burin Asavapibhop Didier Auguste Margherita Buizza Avanzini Andrej Babic Jingzhi Bai Weidong Bai Nikita Balashov Roberto Barbera Andrea Barresi Davide Basilico Eric Baussan Beatrice Bellantonio Marco Bellato JeanLuc Beney Marco Beretta Antonio Bergnoli Enrico Bernieri Nikita Bessonov David Biaré Daniel Bick Lukas Bieger Svetlana Biktemerova Thilo Birkenfeld David Blum Simon Blyth Sara Boarin Manuel Boehles Anastasia Bolshakova Mathieu Bongrand Aurélie Bonhomme Clément Bordereau Matteo Borghesi Augusto Brigatti Timothee Brugiere Riccardo Brugnera Riccardo Bruno Jonas Buchholz Antonio Budano Max Buesken Mario Buscemi Severino Bussino Jose Busto Ilya Butorov Marcel Büchner Anatael Cabrera Barbara Caccianiga Boshuai Cai Hao Cai Xiao Cai Yanke Cai Yi-zhou Cai Zhiyan Cai Stéphane Callier Steven Calvez Antonio Cammi Agustin Campeny Dechang Cai Chuanya Cao Dewen Cao Guofu Cao Jun Cao Yaoqi Cao Rossella Caruso Aurelio Caslini Cédric Cerna Vanessa Cerrone Daniele Cesini Chi Chan Jinfan Chang Yun Chang Milo Charavet Tim Charissé Auttakit Chatrabhuti Chao Chen Guoming Chen Haitao Chen Haotian Chen Jiahui Chen Jian Chen Jing Chen Junyou Chen Lihao Chen Mali Chen Mingming Chen Pingping Chen Po-An Chen Quanyou Chen Shaomin Chen Shenjian Chen Shi Chen Shiqiang Chen Sisi Chen Xin Chen Xuan Chen Xurong Chen Yi-Wen Chen Yiming Chen Yixue Chen Yu Chen Ze Chen Zelin Chen Zhang Chen Zhangming Chen Zhiyuan Chen Zhongchang Chen Zikang Chen Brian Cheng Jie Cheng Yaping Cheng Yu Chin Cheng Zhaokan Cheng Alexander Chepurnov Alexey Chetverikov Davide Chiesa Pietro Chimenti Yen-Ting Chin Pin-Jung Chiu Po-Lin Chou Ziliang Chu Artem Chukanov Neetu Raj Singh Chundawat Anna Chuvashova Gérard Claverie Catia Clementi Barbara Clerbaux Claudio Coletta Marta Colomer Molla Flavio Dal Corso Daniele Corti Salvatore Costa Simon Csakli Chenyang Cui Shanshan Cui Lorenzo Vincenzo D'Auria Olivia Dalager Jaydeep Datta Luis Delgadillo Franco Jiawei Deng Zhi Deng Ziyan Deng Wilfried Depnering Hanna Didenko Xiaoyu Ding Xuefeng Ding Yayun Ding Bayu Dirgantara Carsten Dittrich Sergey Dmitrievsky David Doerflinger Tadeas Dohnal Maria Dolgareva Dmitry Dolzhikov Chuanshi Dong Haojie Dong Jianmeng Dong Lan Dong Damien Dornic Evgeny Doroshkevich Wei Dou Marcos Dracos Olivier Drapier Tobias Drohmann Frédéric Druillole Ran Du Shuxian Du Yujie Duan Katherine Dugas Stefano Dusini Hongyue Duyang Martin Dvorak Jessica Eck Timo Enqvist Heike Enzmann Andrea Fabbri Ulrike Fahrendholz Lukas Fajt Donghua Fan Lei Fan Liangqianjin Fan Can Fang Jian Fang Wenxing Fang Marco Fargetta Elia Stanescu Farilla Anna Fatkina Laurent Favart Dmitry Fedoseev Zhengyong Fei Franz von Feilitzsch Vladko Fekete Li-Cheng Feng Qichun Feng Shaoting Feng Giovanni Ferrante Federico Ferraro Daniela Fetzer Giovanni Fiorentini Andrey Formozov Marcellin Fotzé Amélie Fournier Sabrina Franke Arran Freegard Florian Fritsch Ying Fu Haonan Gan Feng Gao Ruixuan Gao Ruohan Gao Shijiao Gao Alberto Garfagnini Gerard Gaudiot Arsenii Gavrikov Raphaël Gazzini Christoph Genster Diwash Ghimire Marco Giammarchi Agnese Giaz Gianfranco Giordano Nunzio Giudice Franco Giuliani Alexandre Goettel Maxim Gonchar Guanda Gong Guanghua Gong Hui Gong Michel Gonin Oleg Gorchakov Yuri Gornushkin Marco Grassi Christian Grewing Maxim Gromov Vasily Gromov Minhao Gu Xiaofei Gu Yu Gu Mengyun Guan Yuduo Guan Nunzio Guardone Rosa Maria Guizzetti Cong Guo Jingyuan Guo Wanlei Guo Yuhang Guo Paul Hackspacher Caren Hagner Hechong Han Ran Han Xiao Han Yang Han Ziguo Han Chuanhui Hao Jiajun Hao Vidhya Thara Hariharan JinCheng He Jinhong He Miao He Mingtao He Wei He Xinhai He Ziou He Tobias Heinz Dominikus Hellgartner Patrick Hellmuth Shilin Heng Yuekun Heng Rafael Herrera Daojin Hong YuenKeung Hor Shaojing Hou Zhilong Hou Fatima Houria Yee Hsiung Bei-Zhen Hu Hang Hu Hao Hu Jianrun Hu Jun Hu Peng Hu Tao Hu Wei Hu Yuxiang Hu Zhuojun Hu Chunhao Huang Guihong Huang Hanyu Huang Hexiang Huang Jinhao Huang Junlin Huang Junting Huang Kairui Huang Kaixuan Huang Qinhua Huang Shengheng Huang Tao Huang Wenhao Huang Xiaozhong Huang Xin Huang Xingtao Huang Yongbo Huang Lian-Chen Huang Jiaqi Hui Lei Huo Cédric Huss Safeer Hussain Leonard Imbert Antonio Insolia Ara Ioannisian Daniel Ioannisyan Ammad Ul Islam Roberto Isocrate Adrienne Jacobi Arshak Jafar Beatrice Jelmini Kuo-Lun Jen Soeren Jetter Xiangpan Ji Xiaolu Ji Xingzhao Ji Huihui Jia Junji Jia Yi Jia Cailian Jiang Chengbo Jiang Guangzheng Jiang Junjie Jiang Wei Jiang Xiaoshan Jiang Xiaozhao Jiang Yijian Jiang Yixuan Jiang Yue Jiang Ruyi Jin Shuzhu Jin Xiaoping Jing Cécile Jollet Liam Jones Jari Joutsenvaara Sirichok Jungthawan Philipp Kampmann Markus Kaiser Leonidas Kalousis Bowen Kan Li Kang Michael Karagounis Rebin Karaparambil Matej Karas Narine Kazarian Ali Khan Amir Khan Amina Khatun Khanchai Khosonthongkee Florian Kiel Patrick Kinz Denis Korablev Konstantin Kouzakov Alexey Krasnoperov Zinovy Krumshteyn Andre Kruth Tim Kuhlbusch Sergey Kuleshov Sindhujha Kumaran Chun-Hao Kuo Nikolay Kutovskiy Pasi Kuusiniemi Loïc Labit Tobias Lachenmaier Haojing Lai ToUyen LamThi Philipp Landgraf Cecilia Landini Lorenzo Lastrucci Fedor Lazarev Sébastien Leblanc Victor Lebrin Matthieu Lecocq Priscilla Lecomte Frederic Lefevre Liping Lei Ruiting Lei Xiangcui Lei Rupert Leitner Petr Lenskii Jason Leung Bo Li Chao Li Daozheng Li Demin Li Dian Li Fei Li Fule Li Gaoshuang Li Gaosong Li Haitao Li Hongjian Li Huang Li Huiling Li Jiajun Li Jiaqi Li Jin Li Kaijie Li Meiou Li Mengzhao Li Min Li Nan Li Qingjiang Li Quanlin Li Ruhui Li Rui Li Shanfeng Li Shuaijie Li Shuo Li Tao Li Teng Li Weidong Li Weiguo Li Xiaomei Li Xiaonan Li Xiwen Li Xinying Li Yang Li Yawen Li Yi Li Yichen Li Yifan Li Yingke Li Yuanxia Li Yufeng Li Zepeng Li Zhaohan Li Zhibing Li Zhiwei Li Zi-Ming Li Ziyuan Li Zonghai Li An-An Liang Jing Liang Jingjing Liang Jiajun Liao Minghua Liao Yilin Liao Yuzhong Liao Daniel Liebau Ayut Limphirat Sukit Limpijumnong Bo-Chun Lin Guey-Lin Lin Jiming Lin Shengxin Lin Tao Lin Xianhao Lin Xingyi Lin Yen-Hsun Lin Jiacheng Ling Jiajie Ling Xin Ling Ivano Lippi Caimei Liu Fang Liu Fengcheng Liu Gang Liu Haidong Liu Haotian Liu Hongbang Liu Hongjuan Liu Hongtao Liu Hongyang Liu Hu Liu Hui Liu Jianglai Liu Jianli Liu Jiaxi Liu Jin'gao Liu Jinchang Liu Jinyan Liu Kainan Liu Lei Liu Libing Liu Mengchao Liu Menglan Liu Min Liu Qishan Liu Qian Liu Qin Liu Runxuan Liu Shenghui Liu Shuangyu Liu Shubing Liu Shulin Liu Wanjin Liu Xiaowei Liu Ximing Liu Xinkang Liu Xiwen Liu Xuewei Liu Yan Liu Yankai Liu Yin Liu Yiqi Liu Yuanyuan Liu Yuexiang Liu Yunzhe Liu Zhen Liu Zhipeng Liu Zhuo Liu Domenico Lo Presti Salvatore Loffredo Lorenzo Loi Paolo Lombardi Claudio Lombardo Yongbing Long Andrea Longhin Fabio Longhitano Kai Loo Sebastian Lorenz Selma Conforti Di Lorenzo Chuan Lu Fan Lu Haoqi Lu Jiashu Lu Junguang Lu Meishu Lu Peizhi Lu Shuxiang Lu Xianghui Lu Xianguo Lu Xiaoxu Lu Xiaoying Lu Bayarto Lubsandorzhiev Sultim Lubsandorzhiev Livia Ludhova Arslan Lukanov Daibin Luo Fengjiao Luo Guang Luo Jianyi Luo Pengwei Luo Shu Luo Tao Luo Wuming Luo Xiaojie Luo Xiaolan Luo Zhipeng Lv Vladimir Lyashuk Bangzheng Ma Bing Ma Na Ma Qiumei Ma Si Ma Wing Yan Ma Xiaoyan Ma Xubo Ma Santi Maensiri Jingyu Mai Romain Maisonobe Marco Malabarba Yury Malyshkin Roberto Carlos Mandujano Fabio Mantovani Xin Mao Yajun Mao Stefano MMari Cristina Martellini Agnese Martini Jacques Martino Johann Martyn Matthias Mayer Davit Mayilyan Worawat Meevasana Artur Meinusch Qingru Meng Yue Meng Anita Meraviglia Anselmo Meregaglia Emanuela Meroni David Meyhöfer Jian Min Lino Miramonti Nikhil Mohan Salvatore Monforte Paolo Montini Michele Montuschi Nikolay Morozov Iwan Morton-Blake Xiangyi Mu Pavithra Muralidharan Lakshmi Murgod Axel Müller Thomas Mueller Massimiliano Nastasi Dmitry VNaumov Elena Naumova Diana Navas-Nicolas Igor Nemchenok Elisabeth Neuerburg VanHung Nguyen Dennis Nielinger Alexey Nikolaev Feipeng Ning Zhe Ning Yujie Niu Stepan Novikov Hiroshi Nunokawa Lothar Oberauer Juan Pedro Ochoa-Ricoux Samantha Cantu Olea Sebastian Olivares Alexander Olshevskiy Domizia Orestano Fausto Ortica Rainer Othegraven Yifei Pan Alessandro Paoloni Nina Parkalian George Parker Sergio Parmeggiano Achilleas Patsias Teerapat Payupol Viktor Pec Davide Pedretti Yatian Pei Luca Pelicci Nicomede Pelliccia Anguo Peng Haiping Peng Yu Peng Zhaoyuan Peng Elisa Percalli Willy Perrin Frédéric Perrot Pierre-Alexandre Petitjean Fabrizio Petrucci Min Pi Oliver Pilarczyk Ruben Pompilio Artyom Popov Pascal Poussot Stefano Pozzi Wathan Pratumwan Ezio Previtali Sabrina Prummer Fazhi Qi Ming Qi Xiaohui Qi Sen Qian Xiaohui Qian Zhen Qian Liqing Qin Zhonghua Qin Shoukang Qiu Manhao Qu Zhenning Qu Muhammad Usman Rajput Shivani Ramachandran Gioacchino Ranucci Neill Raper Reem Rasheed Thomas Raymond Alessandra Re Henning Rebber Abdel Rebii Bin Ren Shanjun Ren Yuhan Ren Andrea Rendina Cristobal Morales Reveco Taras Rezinko Barbara Ricci Luis Felipe Piñeres Rico Mariam Rifai Markus Robens Mathieu Roche Narongkiat Rodphai Fernanda de Faria Rodrigues Lars Rohwer Aldo Romani Vincent Rompel Bedřich Roskovec Xiangdong Ruan Xichao Ruan Peter Rudakov Saroj Rujirawat Arseniy Rybnikov Andrey Sadovsky Sahar Safari Giuseppe Salamanna Deshan Sandanayake Simone Sanfilippo Anut Sangka Nuanwan Sanguansak Ujwal Santhosh Giuseppe Sava Utane Sawangwit Julia Sawatzki Michaela Schever Jacky Schuler Cédric Schwab Konstantin Schweizer Dmitry Selivanov Alexandr Selyunin Andrea Serafini Giulio Settanta Mariangela Settimo Muhammad Ikram Shahzad Yanjun Shan Junyu Shao Zhuang Shao Anurag Sharma Vladislav Sharov Arina Shaydurova Wei Shen Gang Shi Hangyu Shi Hexi Shi Jingyan Shi Yanan Shi Yongjiu Shi Yuan Shi Dmitrii Shpotya Yike Shu Yuhan Shu She Shuai Vitaly Shutov Andrey Sidorenkov Randhir Singh Apeksha Singhal Chiara Sirignano Jaruchit Siripak Monica Sisti Maciej Slupecki Mikhail Smirnov Oleg Smirnov Thiago Sogo-Bezerra Michael Soiron Sergey Sokolov Julanan Songwadhana Boonrucksar Soonthornthum Felix Sorgenfrei Albert Sotnikov Mario Spinetti Warintorn Sreethawong Achim Stahl Luca Stanco Korbinian Stangler Konstantin Stankevich Hans Steiger Jochen Steinmann Malte Stender Tobias Sterr David Stipp Matthias Raphael Stock Virginia Strati Mikhail Strizh Alexander Studenikin Katharina von Sturm Aoqi Su Jun Su Yuning Su Gongxing Sun Guangbao Sun Hansheng Sun Lijun Sun Liting Sun Mingxia Sun Shifeng Sun Xilei Sun Yongzhao Sun Yunhua Sun Yuning Sun Zhanxue Sun Zhengyang Sun Narumon Suwonjandee Troy Swift Michal Szelezniak DušanŠtefánik FedorŠimkovic OndřejŠrámek Dmitriy Taichenachev Christophe De La Taille Akira Takenaka Hongnan Tan Xiaohan Tan Haozhong Tang Jian Tang Jingzhe Tang Qiang Tang Quan Tang Xiao Tang Jihua Tao Eric Theisen Minh Thuan Nguyen Thi Renju Tian Yuxin Tian Alexander Tietzsch Igor Tkachev Tomas Tmej Marco Danilo Claudio Torri Francesco Tortorici Konstantin Treskov Andrea Triossi Wladyslaw Trzaska Andrei Tsaregorodtsev Alexandros Tsagkarakis Yu-Chen Tung Cristina Tuve Nikita Ushakov Guillaume Vanroyen Nikolaos Vassilopoulos Carlo Venettacci Giuseppe Verde Maxim Vialkov Benoit Viaud Cornelius Moritz Vollbrecht Vit Vorobel Dmitriy Voronin Lucia Votano Stefan van Waasen Stefan Wagner Pablo Walker Jiawei Wan Andong Wang Caishen Wang Chung-Hsiang Wang Cui Wang Derun Wang En Wang Guoli Wang Hanwen Wang Hongxin Wang Huanling Wang Jiabin Wang Jian Wang Jun Wang Ke Wang Kunyu Wang Lan Wang Li Wang Lu Wang Meifen Wang Meng Wang Meng Wang Mingyuan Wang Qianchuan Wang Ruiguang Wang Sibo Wang Siguang Wang Tianhong Wang Tong Wang Wei Wang Wei Wang Wenshuai Wang Wenwen Wang Wenyuan Wang Xi Wang Xiangyue Wang Xuesen Wang Yangfu Wang Yaoguang Wang Yi Wang Yi Wang Yi Wang Yifang Wang Yuanqing Wang Yuman Wang Yuyi Wang Zhe Wang Zheng Wang Zhigang Wang Zhimin Wang Zongyi Wang Apimook Watcharangkool Junya Wei Jushang Wei Lianghong Wei Wei Wei Wei Wei Wenlu Wei Yadong Wei Yuehuan Wei Zhengbao Wei Marcel Weifels Kaile Wen Liangjian Wen Yijie Wen Jun Weng Christopher Wiebusch Rosmarie Wirth Steven Chan-Fai Wong Bjoern Wonsak Baona Wu Bi Wu Chengxin Wu Chia-Hao Wu Chin-Wei Wu Diru Wu Fangliang Wu Jianhua Wu Qun Wu Shuai Wu Wenjie Wu Yinhui Wu Yiyang Wu Zhaoxiang Wu Zhi Wu Zhongyi Wu Michael Wurm Jacques Wurtz Christian Wysotzki Yufei Xi Jingkai Xia Shishen Xian Ziqian Xiang Fei Xiao Pengfei Xiao Tianying Xiao Xiang Xiao Wan Xie Wei-Jun Xie Xiaochuan Xie Yijun Xie Yuguang Xie Zhangquan Xie Zhao Xin Zhizhong Xing Benda Xu Cheng Xu Chuang Xu Donglian Xu Fanrong Xu Hangkun Xu Jiayang Xu Jie Xu Jilei Xu Jinghuan Xu Lingyu Xu Meihang Xu Shiwen Xu Xunjie Xu Ya Xu Yin Xu Yu Xu Dongyang Xue Jingqin Xue Baojun Yan Liangping Yan Qiyu Yan Taylor Yan Tian Yan Wenqi Yan Xiongbo Yan Yupeng Yan Anbo Yang Caihong Yang Changgen Yang Chengfeng Yang Dikun Yang Dingyong Yang Fengfan Yang Haibo Yang Huan Yang Jie Yang Jize Yang Kaiwei Yang Lei Yang Mengting Yang Pengfei Yang Xiaoyu Yang Xuhui Yang Yi Yang Yichen Yang Yifan Yang Yixiang Yang Yujiao Yang Yuzhen Yang Zekun Yang Haifeng Yao Li Yao Jiaxuan Ye Mei Ye Xingchen Ye Ziping Ye Ugur Yegin Frédéric Yermia Peihuai Yi Rattikorn Yimnirun Jilong Yin Na Yin Weiqing Yin Xiangwei Yin Xiaohao Yin Sivaram Yogathasan Zhengyun You Boxiang Yu Chiye Yu Chunxu Yu Guangyou Yu Guojun Yu Hongzhao Yu Miao Yu Peidong Yu Simi Yu Xianghui Yu Yang Yu Zeyuan Yu Zezhong Yu Cenxi Yuan Chengzhuo Yuan Zhaoyang Yuan Zhenxiong Yuan Ziyi Yuan Baobiao Yue Noman Zafar AndréZambanini Jilberto Zamora Matteo Zanetti Vitalii Zavadskyi Fanrui Zeng Pan Zeng Shan Zeng Tingxuan Zeng Yuda Zeng Yujie Zeng Liang Zhan Aiqiang Zhang Bin Zhang Binting Zhang Chengcai Zhang Enze Zhang Feiyang Zhang Guoqing Zhang Haiqiong Zhang Han Zhang Hangchang Zhang Haosen Zhang Honghao Zhang Hongmei Zhang Jialiang Zhang Jiawen Zhang Jie Zhang Jin Zhang Jingbo Zhang Jinnan Zhang Junwei Zhang Kun Zhang Lei Zhang Mingxuan Zhang Mohan Zhang Peng Zhang Ping Zhang Qingmin Zhang Rongping Zhang Rui Zhang Shaoping Zhang Shiqi Zhang Shu Zhang Shuihan Zhang Siyuan Zhang Tao Zhang Xiaofeng Zhang Xiaomei Zhang Xin Zhang Xu Zhang Xuan Zhang Xuantong Zhang Xuesong Zhang Xueyao Zhang Yan Zhang Yibing Zhang Yinhong Zhang Yiyu Zhang Yizhou Zhang Yongjie Zhang Yongpeng Zhang Yu Zhang Yuanyuan Zhang Yue Zhang Yueyuan Zhang Yumei Zhang Yuning Zhang Zhenyu Zhang Zhicheng Zhang Zhijian Zhang Zhixuan Zhang Baoqi Zhao Fengyi Zhao Jie Zhao Liang Zhao Mei Zhao Rong Zhao Runze Zhao Shujun Zhao Tianchi Zhao Tianhao Zhao Yubin Zhao Dongqin Zheng Hua Zheng Xiangyu Zheng Yangheng Zheng Weili Zhong Weirong Zhong Albert Zhou Guorong Zhou Li Zhou Lishui Zhou Min Zhou Shun Zhou Tong Zhou Xiang Zhou Xing Zhou Yan Zhou Haiwen Zhu Jiang Zhu Jingsen Zhu Jingyu Zhu Kangfu Zhu Kejun Zhu Zhihang Zhu Ivan Zhutikov Bo Zhuang Honglin Zhuang Liang Zong Jiaheng Zou Sebastian Zwickel Jan Züfle JUNO Collaboration 《Chinese Physics C》 SCIE CAS CSCD 2026年第4期1-31,共31页

The Jiangmen Underground Neutrino Observatory(JUNO)started physics data taking on 26 August 2025.JUNO consists of a 20-kton liquid scintillator central detector,surrounded by a 35 kton water pool serving as a Cherenko... The Jiangmen Underground Neutrino Observatory(JUNO)started physics data taking on 26 August 2025.JUNO consists of a 20-kton liquid scintillator central detector,surrounded by a 35 kton water pool serving as a Cherenkov veto,and almost 1000 m² of plastic scintillator veto on top.The detector is located in a shallow underground laboratory with an overburden of 1800 m.w.e.This paper presents the performance results of the detector,extensively studied during the commissioning of the water phase,the subsequent liquid scintillator filling phase,and the first physics runs.The liquid scintillator achieved an attenuation length of 20.6 m at 430 nm,while the high coverage PMT system and scintillator together yielded about 1785 photoelectrons per MeV of energy deposit at the detector centre,measured using the 2.223 MeVγfrom neutron captures on hydrogen with an Am-C calibration source.The reconstructed energy resolution is 3.4%for two 0.511 MeVγat the detector centre and 2.9%for the 0.93 MeV quenched ²¹⁴Po alpha decays from natural radioactive sources.The energy non-linearity is calibrated to better than 1%.Intrinsic contaminations of ²³⁸U and ²³²Th in the liquid scintillator are below 10^-16 g/g,assuming secular equilibrium.The water Cherenkov detector achieves a muon detection efficiency better than 99.9%for muons traversing the liquid scintillator volume.During the initial science runs,the data acquisition duty cycle exceeded 97.8%,demonstrating the excellent stability and readiness of JUNO for high-precision neutrino physics. 展开更多

关键词 neutrino oscillations JUNO detector performance

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Prediction of energy resolution in the JUNO experiment 认领 引用 被引量：1

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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》 SCIE CAS CSCD 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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Potential to identify neutrino mass ordering with reactor antineutrinos at JUNO 认领 引用 被引量：1

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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》 SCIE CAS CSCD 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 angleθ₂₃.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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Combined FOLFOX4 with all-trans retinoic acid versus FOLFOX4 with placebo in treatment of advanced hepatocellular carcinoma with extrahepatic metastasis: a randomized, double-blind comparative study 认领 引用 被引量：16

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作者 Juxian Sun Feifei Mao +8 位作者 Chang Liu Fan Zhang Dafeng Jiang Weixing Guo Lei Huo Liping Zhou Wan Yee Lau Jie Shi Shuqun Cheng 《Signal Transduction and Targeted Therapy》 SCIE CSCD 2023年第10期5096-5105,共10页

The majority of hepatocellular carcinoma(HCC)cases are diagnosed at an advanced stage.Currently,there are only a few therapeutic methods available for patients with advanced HCC and extrahepatic metastasis(EHM).System... The majority of hepatocellular carcinoma(HCC)cases are diagnosed at an advanced stage.Currently,there are only a few therapeutic methods available for patients with advanced HCC and extrahepatic metastasis(EHM).Systemic chemotherapy,such as FOLFOX4(infusions of fluorouracil,leucovorin,and oxaliplatin),has been reported for treating advanced HCC with EHM,but its effectiveness is very poor. 展开更多

关键词 FOLFOX4 metastasis chemotherapy

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JUNO sensitivity on proton decay p→νK⁺searches 认领 引用 被引量：2

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作者 Nikolay Anfimov Angel Abusleme +609 位作者 Thomas Adam Shakeel Ahmad Rizwan Ahmed Sebastiano Aiello Muhammad Akram Fengpeng An Qi An Giuseppe Andronico Nikolay Anfimov Vito Antonelli Tatiana Antoshkina Burin Asavapibhop João Pedro Athayde Marcondes de André Didier Auguste Nikita Balashov Wander Baldini Andrea Barresi Davide Basilico Eric Baussan Marco Bellato Antonio Bergnoli Thilo Birkenfeld Sylvie Blin David Blum Simon Blyth Anastasia Bolshakova Mathieu Bongrand Clément Bordereau Dominique Breton Augusto Brigatti Riccardo Brugnera Riccardo Bruno Antonio Budano Mario Buscemi Jose Busto Ilya Butorov Anatael Cabrera Barbara Caccianiga Hao Cai Xiao Cai Yanke Cai Zhiyan Cai Riccardo Callegari Antonio Cammi Agustin Campeny Chuanya Cao Guofu Cao Jun Cao Rossella Caruso Cédric Cerna Jinfan Chang Yun Chang Pingping Chen Po-An Chen Shaomin Chen Xurong Chen Yi-Wen Chen Yixue Chen Yu Chen Zhang Chen Jie Cheng Yaping Cheng Alexey Chetverikov Davide Chiesa Pietro Chimenti Artem Chukanov Gérard Claverie Catia Clementi Barbara Clerbaux Selma Conforti Di Lorenzo Daniele Corti Flavio Dal Corso Olivia Dalager Christophe De La Taille Zhi Deng Ziyan Deng Wilfried Depnering Marco Diaz Xuefeng Ding Yayun Ding Bayu Dirgantara Sergey Dmitrievsky Tadeas Dohnal Dmitry Dolzhikov Georgy Donchenko Jianmeng Dong Evgeny Doroshkevich Marcos Dracos Frédéric Druillole Ran Du Shuxian Du Stefano Dusini Martin Dvorak Timo Enqvist Heike Enzmann Andrea Fabbri Ulrike Fahrendholz Donghua Fan Lei Fan Jian Fang Wenxing Fang Marco Fargetta Dmitry Fedoseev Li-Cheng Feng Qichun Feng Richard Ford Amélie Fournier Haonan Gan Feng Gao Alberto Garfagnini Arsenii Gavrikov Marco Giammarchi Agnese Giaz Nunzio Giudice Maxim Gonchar Guanghua Gong Hui Gong Yuri Gornushkin Alexandre Göttel Marco Grassi Christian Grewing Vasily Gromov Minghao Gu Xiaofei Gu Yu Gu Mengyun Guan Nunzio Guardone Maria Gul Cong Guo Jingyuan Guo Wanlei Guo Xinheng Guo Yuhang Guo Paul Hackspacher Caren Hagner Ran Han Yang Han Muhammad Sohaib Hassan 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 Chunhao Huang Guihong Huang Hanxiong Huang Wenhao Huang Xin Huang Xingtao Huang Yongbo Huang Jiaqi Hui Lei Huo Wenju Huo Cédric Huss Safeer Hussain Ara Ioannisian Roberto Isocrate Beatrice Jelmini Kuo-Lun Jen Ignacio Jeria Xiaolu Ji Xingzhao Ji Huihui Jia Junji Jia Siyu Jian Di Jiang Wei Jiang Xiaoshan Jiang Ruyi Jin Xiaoping Jing Cécile Jollet Jari Joutsenvaara Sirichok Jungthawan Leonidas Kalousis Philipp Kampmann Li Kang Rebin Karaparambil Narine Kazarian Amina Khatun Khanchai Khosonthongkee Denis Korablev Konstantin Kouzakov Alexey Krasnoperov Andre Kruth Nikolay Kutovskiy Pasi Kuusiniemi Tobias Lachenmaier Cecilia Landini Sébastien Leblanc Victor Lebrin Frederic Lefevre Ruiting Lei Rupert Leitner Jason Leung Demin Li Fei Li Fule Li Gaosong Li Haitao Li Huiling Li Jiaqi Li Mengzhao Li Min Li Nan Li Nan Li Qingjiang Li Ruhui Li Shanfeng Li Tao Li Weidong Li Weiguo Li Xiaomei Li Xiaonan Li Xinglong Li Yi Li Yichen Li Yufeng Li Zhaohan Li Zhibing Li Ziyuan Li Hao Liang Hao Liang Jiajun Liao Daniel Liebau Ayut Limphirat Sukit Limpijumnong Guey-Lin Lin Shengxin Lin Tao Lin Jiajie Ling Ivano Lippi Fang Liu Haidong Liu Hongbang Liu Hongjuan Liu Hongtao Liu Hui Liu Jianglai Liu Jinchang Liu Min Liu Qian Liu Qin Liu Runxuan Liu Shuangyu Liu Shubin Liu Shulin Liu Xiaowei Liu Xiwen Liu Yan Liu Yunzhe Liu Alexey Lokhov Paolo Lombardi Claudio Lombardo Kai Loo Chuan Lu Haoqi Lu Jingbin Lu Junguang Lu Shuxiang Lu Xiaoxu Lu Bayarto Lubsandorzhiev Sultim Lubsandorzhiev Livia Ludhova Arslan Lukanov Fengjiao Luo Guang Luo Pengwei Luo Shu Luo Wuming Luo Vladimir Lyashuk Bangzheng Ma Qiumei Ma Si Ma Xiaoyan Ma Xubo Ma Jihane Maalmi Yury Malyshkin Roberto Carlos Mandujano Fabio Mantovani Francesco Manzali Xin Mao Yajun Mao Stefano M.Mari Filippo Marini Sadia Marium Cristina Martellini Gisele Martin-Chassard Agnese Martini Matthias Mayer Davit Mayilyan Ints Mednieks Yue Meng Anselmo Meregaglia Emanuela Meroni David Meyhöfer Mauro Mezzetto Jonathan Miller Lino Miramonti Paolo Montini Michele Montuschi Axel Müller Massimiliano Nastasi Dmitry V.Naumov Elena Naumova Diana Navas-Nicolas Igor Nemchenok Minh Thuan Nguyen Thi 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 Nicomede Pelliccia Anguo Peng Haiping Peng Frédéric Perrot Pierre-Alexandre Petitjean Fabrizio Petrucci Oliver Pilarczyk Luis Felipe Piñeres Rico Artyom Popov Pascal Poussot Wathan Pratumwan Ezio Previtali Fazhi Qi Ming Qi Sen Qian Xiaohui Qian Zhen Qian Hao Qiao Zhonghua Qin Shoukang Qiu Muhammad Usman Rajput Gioacchino Ranucci Neill Raper Alessandra Re Henning Rebber Abdel Rebii Bin Ren Jie Ren Barbara Ricci Mariam Rifai Markus Robens Mathieu Roche Narongkiat Rodphai Aldo Romani Bedřich Roskovec Christian Roth Xiangdong Ruan Xichao Ruan Saroj Rujirawat Arseniy Rybnikov Andrey Sadovsky Paolo Saggese Simone Sanfilippo Anut Sangka Nuanwan Sanguansak Utane Sawangwit Julia Sawatzki Fatma Sawy Michaela Schever Cédric Schwab Konstantin Schweizer Alexandr Selyunin Andrea Serafini Giulio Settanta Mariangela Settimo Zhuang Shao Vladislav Sharov Arina Shaydurova Jingyan Shi Yanan Shi Vitaly Shutov Andrey Sidorenkov FedorŠimkovic Chiara Sirignano Jaruchit Siripak Monica Sisti Maciej Slupecki Mikhail Smirnov Oleg Smirnov Thiago Sogo-Bezerra Sergey Sokolov Julanan Songwadhana Boonrucksar Soonthornthum Albert Sotnikov OndřejŠrámek Warintorn Sreethawong Achim Stahl Luca Stanco Konstantin Stankevich DušanŠtefánik Hans Steiger Jochen Steinmann Tobias Sterr Matthias Raphael Stock Virginia Strati Alexander Studenikin Shifeng Sun Xilei Sun Yongjie Sun Yongzhao Sun Narumon Suwonjandee Michal Szelezniak Jian Tang Qiang Tang Quan Tang Xiao Tang Alexander Tietzsch Igor Tkachev Tomas Tmej Marco Danilo Claudio Torri Konstantin Treskov Andrea Triossi Giancarlo Troni Wladyslaw Trzaska Cristina Tuve Nikita Ushakov Johannes van den Boom Stefan van Waasen Guillaume Vanroyen Vadim Vedin Giuseppe Verde Maxim Vialkov Benoit Viaud Cornelius Moritz Vollbrecht Cristina Volpe Vit Vorobel Dmitriy Voronin Lucia Votano Pablo Walker Caishen Wang Chung-Hsiang Wang En Wang Guoli Wang Jian Wang Jun Wang Kunyu Wang Lu Wang Meifen Wang Meng Wang Meng Wang Ruiguang Wang Siguang Wang Wei Wang Wei Wang Wenshuai Wang Xi Wang Xiangyue Wang Yangfu Wang Yaoguang Wang Yi Wang Yi Wang Yifang Wang Yuanqing Wang Yuman Wang Zhe Wang Zheng Wang Zhimin Wang Zongyi Wang Muhammad Waqas Apimook Watcharangkool Lianghong Wei Wei Wei Wenlu Wei Yadong Wei Kaile Wen Liangjian Wen Christopher Wiebusch Steven Chan-Fai Wong Bjoern Wonsak Diru Wu Qun Wu Zhi Wu Michael Wurm Jacques Wurtz Christian Wysotzki Yufei Xi Dongmei Xia Xiang Xiao Xiaochuan Xie Yuguang Xie Zhangquan Xie Zhizhong Xing Benda Xu Cheng Xu Donglian Xu Fanrong Xu Hangkun Xu Jilei Xu Jing Xu Meihang Xu Yin Xu Yu Xu Baojun Yan Taylor Yan Wenqi Yan Xiongbo Yan Yupeng Yan Anbo Yang Changgen Yang Chengfeng Yang Huan Yang Jie Yang Lei Yang Xiaoyu Yang Yifan Yang Yifan Yang Haifeng Yao Zafar Yasin Jiaxuan Ye Mei Ye Ziping Ye Ugur Yegin Frédéric Yermia Peihuai Yi Na Yin Xiangwei Yin Zhengyun You Boxiang Yu Chiye Yu Chunxu Yu Hongzhao Yu Miao Yu Xianghui Yu Zeyuan Yu Zezhong Yu Chengzhuo Yuan Ying Yuan Zhenxiong Yuan Baobiao Yue Noman Zafar Andre Zambanini Vitalii Zavadskyi Shan Zeng Tingxuan Zeng Yuda Zeng Liang Zhan Aiqiang Zhang Feiyang Zhang Guoqing Zhang Haiqiong Zhang Honghao Zhang Jialiang Zhang Jiawen Zhang Jie Zhang Jin Zhang Jingbo Zhang Jinnan Zhang Peng Zhang Qingmin Zhang Shiqi Zhang Shu Zhang Tao Zhang Xiaomei Zhang Xin Zhang Xuantong Zhang Xueyao Zhang Yan Zhang Yinhong Zhang Yiyu Zhang Yongpeng Zhang Yu Zhang Yuanyuan Zhang Yumei Zhang Zhenyu Zhang Zhijian Zhang Fengyi Zhao Jie Zhao Rong Zhao Shujun Zhao Tianchi Zhao Dongqin Zheng Hua Zheng Yangheng Zheng Weirong Zhong Jing Zhou Li Zhou Nan Zhou Shun Zhou Tong Zhou Xiang Zhou Jiang Zhu Kangfu Zhu Kejun Zhu Zhihang Zhu Bo Zhuang Honglin Zhuang Liang Zong Jiaheng Zou JUNO Collaboration 《Chinese Physics C》 SCIE CAS CSCD 2023年第11期7-22,共16页

The Jiangmen Underground Neutrino Observatory(JUNO)is a large liquid scintillator detector designed to explore many topics in fundamental physics.In this study,the potential of searching for proton decay in the p→νK... The Jiangmen Underground Neutrino Observatory(JUNO)is a large liquid scintillator detector designed to explore many topics in fundamental physics.In this study,the potential of searching for proton decay in the p→νK⁺mode with JUNO is investigated.The kaon and its decay particles feature a clear three-fold coincidence signature that results in a high efficiency for identification.Moreover,the excellent energy resolution of JUNO permits suppression of the sizable background caused by other delayed signals.Based on these advantages,the detection efficiency for the proton decay via p→νK⁺is 36.9%±4.9%with a background level of 0.2±0.05(syst)±0.2(stat)events after 10 years of data collection.The estimated sensitivity based on 200 kton-years of exposure is 9.6×1033 years,which is competitive with the current best limits on the proton lifetime in this channel and complements the use of different detection technologies. 展开更多

关键词 proton decay grand unified theories JUNO liquid scintillator detector

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Sub-percent precision measurement of neutrino oscillation parameters with JUNO 认领 引用 被引量：5

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作者 Angel Abusleme Thomas Adam +601 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 Antonio Bergnoli Thilo Birkenfeld Sylvie Blin David Blum Simon Blyth Anastasia Bolshakova Mathieu Bongrand Clément Bordereau Dominique Breton Augusto Brigatti Riccardo Brugnera Riccardo Bruno Antonio Budano Jose Busto Ilya Butorov Anatael Cabrera Barbara Caccianiga Hao Cai Xiao Cai Yanke Cai Zhiyan Cai Riccardo Callegari Antonio Cammi Agustin Campeny Chuanya Cao Guofu Cao Jun Cao Rossella Caruso Cédric Cerna Chi Chan Jinfan Chang Yun Chang Guoming Chen Pingping Chen Po-An Chen Shaomin Chen Xurong Chen Yixue Chen Yu Chen Zhiyuan Chen Zikang Chen Jie Cheng Yaping Cheng Yu Chin Cheng Alexey Chetverikov Davide Chiesa Pietro Chimenti Artem Chukanov Gérard Claverie Catia Clementi Barbara Clerbaux Selma Conforti Di Lorenzo Daniele Corti Flavio Dal Corso Olivia Dalager Christophe De La Taille Zhi Deng Ziyan Deng Wilfried Depnering Marco Diaz Xuefeng Ding Yayun Ding Bayu Dirgantara Sergey Dmitrievsky Tadeas Dohnal Dmitry Dolzhikov Georgy Donchenko Jianmeng Dong Evgeny Doroshkevich Marcos Dracos Frédéric Druillole Ran Du Shuxian Du Stefano Dusini Martin Dvorak Timo Enqvist Heike Enzmann Andrea Fabbri Donghua Fan Lei Fan Jian Fang Wenxing Fang Marco Fargetta Dmitry Fedoseev Zhengyong Fei Li-Cheng Feng Qichun Feng Richard Ford Amélie Fournier Haonan Gan Feng Gao Alberto Garfagnini Arsenii Gavrikov Marco Giammarchi Nunzio Giudice Maxim Gonchar Guanghua Gong Hui Gong Yuri Gornushkin Alexandre Göttel Marco Grassi Vasily Gromov Minghao Gu Xiaofei Gu Yu Gu Mengyun Guan Yuduo Guan Nunzio Guardone Cong Guo Jingyuan Guo Wanlei Guo Xinheng Guo Yuhang Guo Paul Hackspacher 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 Kaixuan Huang Wenhao Huang Xin Huang Xingtao Huang Yongbo Huang Jiaqi Hui Lei Huo Wenju Huo Cédric Huss Safeer Hussain Ara Ioannisian Roberto Isocrate Beatrice Jelmini Ignacio Jeria Xiaolu Ji Huihui Jia Junji Jia Siyu Jian Di Jiang Wei Jiang Xiaoshan Jiang Xiaoping Jing Cécile Jollet Jari Joutsenvaara Leonidas Kalousis Philipp Kampmann Li Kang Rebin Karaparambil Narine Kazarian Amina Khatun Khanchai Khosonthongkee Denis Korablev Konstantin Kouzakov Alexey Krasnoperov Nikolay Kutovskiy Pasi Kuusiniemi Tobias Lachenmaier Cecilia Landini Sébastien Leblanc Victor Lebrin Frederic Lefevre Ruiting Lei Rupert Leitner Jason Leung Daozheng Li Demin Li Fei Li Fule Li Gaosong Li Huiling Li Mengzhao Li Min Li Nan 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 Zepeng 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 Ivano Lippi Fang Liu Haidong Liu Haotian Liu Hongbang Liu Hongjuan Liu Hongtao Liu Hui Liu Jianglai Liu Jinchang Liu Min Liu Qian Liu Qin Liu Runxuan Liu Shubin Liu Shulin Liu Xiaowei Liu Xiwen Liu Yan Liu Yunzhe Liu Alexey Lokhov Paolo Lombardi Claudio Lombardo Kai Loo Chuan Lu Haoqi Lu Jingbin Lu Junguang Lu Shuxiang Lu Bayarto Lubsandorzhiev Sultim Lubsandorzhiev Livia Ludhova Arslan Lukanov Daibin Luo Fengjiao Luo Guang 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 Yury Malyshkin Roberto Carlos Mandujano Fabio Mantovani Francesco Manzali Xin Mao Yajun Mao Stefano M.Mari Filippo Marini Cristina Martellini Gisele Martin-Chassard Agnese Martini Matthias Mayer Davit Mayilyan Ints Mednieks Artur Meinusch Yue Meng Anselmo Meregaglia Emanuela Meroni David Meyhö Mauro Mezzetto Jonathan Miller Lino Miramonti Marta Colomer Molla Paolo Montini Michele Montuschi Axel Müller Massimiliano Nastasi Dmitry V.Naumov Elena Naumova Diana Navas-Nicolas Igor Nemchenok Minh Thuan Nguyen Thi 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 Nicomede Pelliccia Anguo Peng Haiping Peng Yu Peng Zhaoyuan Peng Frédéric Perrot Pierre-Alexandre Petitjean Fabrizio Petrucci Oliver Pilarczyk Luis Felipe Piñeres Artyom Popov Pascal Poussot Ezio Previtali Fazhi Qi Ming Qi Sen Qian Xiaohui Qian Zhen Qian Hao Qiao Zhonghua Qin Shoukang Qiu Gioacchino Ranucci Neill Raper Reem Rasheed Alessandra Re Henning Rebber Abdel Rebii Mariia Redchuk Bin Ren Jie Ren Barbara Ricci Mariam Rifai Mathieu Roche Narongkiat Rodphai Aldo Romani Bedřich Roskovec Xichao Ruan Arseniy Rybnikov Andrey Sadovsky Paolo Saggese Simone Sanfilippo Anut Sangka Utane Sawangwit Julia Sawatzki Michaela Schever Cédric Schwab Konstantin Schweizer Alexandr Selyunin Andrea Serafini Giulio Settanta Mariangela Settimo Zhuang Shao Vladislav Sharov Arina Shaydurova Jingyan Shi Yanan Shi Vitaly Shutov Andrey Sidorenkov FedorŠimkovic Chiara Sirignano Jaruchit Siripak Monica Sisti Maciej Slupecki Mikhail Smirnov Oleg Smirnov Thiago Sogo-Bezerra Sergey Sokolov Julanan Songwadhana Boonrucksar Soonthornthum Albert Sotnikov OndřejŠrámek Warintorn Sreethawong Achim Stahl Luca Stanco Konstantin Stankevich DušanŠtefánik Hans Steiger Jochen Steinmann Tobias Sterr Matthias Raphael Stock Virginia Strati Alexander Studenikin Jun Su Shifeng Sun Xilei Sun Yongjie Sun Yongzhao Sun Zhengyang Sun Narumon Suwonjandee Michal Szelezniak Jian Tang Qiang Tang Quan Tang Xiao Tang Vidhya Thara Hariharan Eric Theisen Alexander Tietzsch Igor Tkachev Tomas Tmej Marco Danilo Claudio Torri Konstantin Treskov Andrea Triossi Giancarlo Troni Wladyslaw Trzaska Alexandros Tsagkarakis Cristina Tuve Nikita Ushakov Vadim Vedin Giuseppe Verde Maxim Vialkov Benoit Viaud Cornelius Moritz Vollbrecht Cristina Volpe Katharina Von Sturm Vit Vorobel Dmitriy Voronin Lucia Votano Pablo Walker Caishen Wang Chung-Hsiang Wang En Wang Guoli Wang Jian Wang Jun Wang Lu Wang Meifen Wang Meng Wang Meng Wang Ruiguang Wang Siguang Wang Wei Wang Wei Wang Wenshuai Wang Xi Wang Xiangyue Wang Yangfu Wang Yaoguang Wang Yi Wang Yi Wang Yifang Wang Yuanqing Wang Yuman Wang Zhe Wang Zheng Wang Zhimin Wang Zongyi Wang Apimook Watcharangkool Wei Wei Wei Wei Wenlu Wei Yadong Wei Kaile Wen Liangjian Wen Christopher Wiebusch Steven Chan-Fai Wong Bjoern Wonsak Diru Wu Qun Wu Zhi Wu Michael Wurm Jacques Wurtz Christian Wysotzki Yufei Xi Dongmei Xia 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 Yin Xu Baojun Yan Taylor Yan Wenqi Yan Xiongbo Yan Yupeng Yan Changgen Yang Chengfeng Yang Huan Yang Jie Yang Lei Yang Xiaoyu Yang Yifan Yang Haifeng Yao Jiaxuan Ye Mei Ye Ziping Ye Frédéric Yermia Na Yin Zhengyun You Boxiang Yu Chiye Yu Chunxu Yu Hongzhao Yu Miao Yu Xianghui Yu Zeyuan Yu Zezhong Yu Cenxi Yuan Chengzhuo Yuan Ying Yuan Zhenxiong Yuan Baobiao Yue Noman Zafar Vitalii Zavadskyi Shan Zeng Tingxuan Zeng Yuda Zeng Liang Zhan Aiqiang Zhang Bin Zhang Binting Zhang Feiyang Zhang Guoqing Zhang Honghao Zhang Jialiang Zhang Jiawen Zhang Jie Zhang Jin Zhang Jingbo Zhang Jinnan Zhang Mohan Zhang Peng Zhang Qingmin Zhang Shiqi Zhang Shu Zhang Tao Zhang Xiaomei Zhang Xin Zhang Xuantong Zhang Xueyao Zhang Yinhong Zhang Yiyu Zhang Yongpeng Zhang Yu Zhang Yuanyuan Zhang Yumei Zhang Zhenyu Zhang Zhijian Zhang Fengyi Zhao 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 Jiang Zhu Jingsen Zhu Kangfu Zhu Kejun Zhu Zhihang Zhu Bo Zhuang Honglin Zhuang Liang Zong Jiaheng Zou 《Chinese Physics C》 SCIE CAS CSCD 2022年第12期28-49,共22页

JUNO is a multi-purpose neutrino observatory under construction in the south of China.This publication presents new sensitivity estimates for the measurement of the△m₃₁²,△m₂₁²,sin²θ₁₂,and sin²... JUNO is a multi-purpose neutrino observatory under construction in the south of China.This publication presents new sensitivity estimates for the measurement of the△m₃₁²,△m₂₁²,sin²θ₁₂,and sin²θ₁₃oscillation parameters using reactor antineutrinos,which is one of the primary physics goals of the experiment.The sensitivities are obtained using the best knowledge available to date on the location and overburden of the experimental site,the nuclear reactors in the surrounding area and beyond,the detector response uncertainties,and the reactor antineutrino spectral shape constraints expected from the TAO satellite detector.It is found that the△m₂₁²and sin²θ₁₂oscillation parameters will be determined to 0.5%precision or better in six years of data collection.In the same period,the△m₃₁²parameter will be determined to about 0.2%precision for each mass ordering hypothesis.The new precision represents approximately an order of magnitude improvement over existing constraints for these three parameters. 展开更多

关键词 neutrino oscillation reactor antineutrino precision measurement JUNO

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A Noninvasive Approach to Evaluate Tumor Immune Microenvironment and Predict Outcomes in Hepatocellular Carcinoma 认领 引用 被引量：6

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作者 Jianmin Wu Wanmin Liu +9 位作者 Xinyao Qiu Jing Li Kairong Song Siyun Shen Lei Huo Lu Chen Mingshuang Xu Hongyang Wang Ningyang Jia Lei Chen 《Phenomics》 2023年第6期549-564,共16页

It is widely recognized that tumor immune microenvironment(TIME)plays a crucial role in tumor progression,metastasis,and therapeutic response.Despite several noninvasive strategies have emerged for cancer diagnosis an... It is widely recognized that tumor immune microenvironment(TIME)plays a crucial role in tumor progression,metastasis,and therapeutic response.Despite several noninvasive strategies have emerged for cancer diagnosis and prognosis,there are still lack of efective radiomic-based model to evaluate TIME status,let alone predict clinical outcome and immune checkpoint inhibitor(ICIs)response for hepatocellular carcinoma(HCC).In this study,we developed a radiomic model to evaluate TIME status within the tumor and predict prognosis and immunotherapy response.A total of 301 patients who underwent magnetic resonance imaging(MRI)examinations were enrolled in our study.The intra-tumoral expression of 17 immune-related molecules were evaluated using co-detection by indexing(CODEX)technology,and we construct Immunoscore(IS)with the least absolute shrinkage and selection operator(LASSO)algorithm and Cox regression method to evaluate TIME.Of 6115 features extracted from MRI,fve core features were fltered out,and the Radiomic Immunoscore(RIS)showed high accuracy in predicting TIME status in testing cohort(area under the curve=0.753).More importantly,RIS model showed the capability of predicting therapeutic response to anti-programmed cell death 1(PD-1)immunotherapy in an independent cohort with advanced HCC patients(area under the curve=0.731).In comparison with previously radiomicbased models,our integrated RIS model exhibits not only higher accuracy in predicting prognosis but also the potential guiding signifcance to HCC immunotherapy. 展开更多

关键词 Hepatocellular carcinoma Tumor immune microenvironment Radiomic Prognosis Immunotherapy response

Single-particle space-momentum angle distribution effect on two-pion HBT correlation in high-energy heavy-ion collisions 认领 引用

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作者 Hang Yang Qichun Feng +2 位作者 Yanyv Ren Jingbo Zhang Lei Huo 《Chinese Physics C》 SCIE CAS CSCD 2020年第5期78-86,共9页

We analyze the transverse momentum dependence of HBT radii in relativistic heavy-ion collisions using several source models.Results indicate that the single-particle space-momentum angle distribution plays an importan... We analyze the transverse momentum dependence of HBT radii in relativistic heavy-ion collisions using several source models.Results indicate that the single-particle space-momentum angle distribution plays an important role in the transverse momentum dependence of HBT radii.In a cylinder source,we use several formulas to describe the transverse momentum dependence of HBT radii and the single-particle space-momentum angle distribution.We also make a numerical connection between them in the transverse plane. 展开更多

关键词 HBT radii transverse momentum dependence space-momentum angle distribution

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