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A ROOT-based detector geometry and event visualization system for JUNO-TAO
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作者 Ming-Hua Liao Kai-Xuan Huang +3 位作者 Yu-Mei Zhang Jia-Yang Xu Guo-Fu Cao Zheng-Yun You 《Nuclear Science and Techniques》 2025年第3期50-59,共10页
The Taishan Antineutrino Observatory(TAO)is a satellite experiment of the Jiangmen Underground Neutrino Observatory,located near the Taishan nuclear power plant(NPP).The TAO aims to measure the energy spectrum of reac... The Taishan Antineutrino Observatory(TAO)is a satellite experiment of the Jiangmen Underground Neutrino Observatory,located near the Taishan nuclear power plant(NPP).The TAO aims to measure the energy spectrum of reactor antineutrinos with unprecedented precision,which would benefit both reactor neutrino physics and the nuclear database.A detector geometry and event visualization system was developed for the TAO.The software was based on ROOT packages and embedded in the TAO offline software framework.This provided an intuitive tool for visualizing the detector geometry,tuning the reconstruction algorithm,understanding neutrino physics,and monitoring the operation of reactors at NPP.Further applications of the visualization system in the experimental operation of TAO and its future development are discussed. 展开更多
关键词 Visualization GEOMETRY Offline software juno TAO
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Sub-GeV events energy reconstruction with 3-inch PMTs in JUNO
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作者 Si-Yuan Zhang Yong-Bo Huang +2 位作者 Miao He Cheng-Feng Yang Guo-Ming Chen 《Nuclear Science and Techniques》 2025年第5期88-101,共14页
A 20-kiloton liquid scintillator detector is under construction at the Jiangmen Underground Neutrino Observatory(JUNO)for several physics purposes.Detecting neutrinos released from nuclear reactors,the sun,supernova b... A 20-kiloton liquid scintillator detector is under construction at the Jiangmen Underground Neutrino Observatory(JUNO)for several physics purposes.Detecting neutrinos released from nuclear reactors,the sun,supernova bursts,and Earth's atmosphere across a wide energy range necessitates efficient reconstruction algorithms.In this study,we introduce a novel method for reconstructing event energy by counting 3-inch photomultiplier tubes(PMTs)with or without signals.The proposed algorithm demonstrated excellent performance in accurate energy reconstruction,validated with electron Monte Carlo samples covering kinetic energies ranging from 10 MeV to 1 GeV. 展开更多
关键词 Energy reconstruction Liquid scintillator detectors juno OCCUPANCY method
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Izumo1和Juno在哺乳动物受精过程中的研究进展 被引量:2
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作者 胡文萍 汤继顺 +5 位作者 张壮彪 喇永富 刘秋月 狄冉 王翔宇 储明星 《畜牧兽医学报》 CAS CSCD 北大核心 2019年第9期1539-1547,共9页
受精是哺乳动物一个精确而且高度协调的生理过程。精子与卵子的融合是其中最关键的一步。两个高度分化的单倍体生殖细胞,精子和卵子,通过融合形成一个全新的受精卵,并发育为胚胎。Izumo1和Juno是目前发现的第一个精子和卵子质膜上的配体... 受精是哺乳动物一个精确而且高度协调的生理过程。精子与卵子的融合是其中最关键的一步。两个高度分化的单倍体生殖细胞,精子和卵子,通过融合形成一个全新的受精卵,并发育为胚胎。Izumo1和Juno是目前发现的第一个精子和卵子质膜上的配体-受体蛋白对,它们的相互作用是精卵识别所必须的。本文综述了这两种重要蛋白的发现及它们在精卵融合过程中的相互作用,同时阐述了哺乳动物受精过程的最新研究进展。 展开更多
关键词 juno Izumo1 精卵融合 受精 顶体反应
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Trimble Juno SB手持机结合ArcPad软件在城市规划调查研究中的应用 被引量:4
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作者 周爱华 付晓 《北京联合大学学报》 CAS 2012年第3期21-25,共5页
城市规划调查研究是城市规划工作的基础。随着GPS定位精度的提高,手持GPS成功应用于城市规划调查研究。介绍了Trimble Juno SB手持机配合ArcPad软件在城市规划调查研究各个阶段的具体应用,总结了手持GPS应用于城市规划调查研究的优劣势... 城市规划调查研究是城市规划工作的基础。随着GPS定位精度的提高,手持GPS成功应用于城市规划调查研究。介绍了Trimble Juno SB手持机配合ArcPad软件在城市规划调查研究各个阶段的具体应用,总结了手持GPS应用于城市规划调查研究的优劣势,并就未来发展进行了展望。 展开更多
关键词 城市规划调查研究 手持GPS TRIMBLE juno SB ARCPAD
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Expression of Ferric Chelate Reductase Gene in Citrus junos and Poncirus trifoliataTissues 被引量:1
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作者 李凌 范艳华 +2 位作者 罗小英 裴炎 周泽扬 《Acta Botanica Sinica》 CSCD 2002年第7期771-774,共4页
It has been hypothesized that under iron stress high ferric chelate reductase (FCR) activity in the absorptive root of plants tolerant to iron_deficiency will be induced and result in subsequent Fe 2+ transport a... It has been hypothesized that under iron stress high ferric chelate reductase (FCR) activity in the absorptive root of plants tolerant to iron_deficiency will be induced and result in subsequent Fe 2+ transport across the plasmalemma. The activity of FCR and expression of FCR gene (FRO2) in Citrus junos Sieb. ex Tanaka tolerant to iron_deficiency and Poncirus trifoliata (L.) Raf. susceptible to iron_deficiency were determined to elucidate the physiological difference which causes the different tolerance of the two citrus rootstocks to iron stress. The activity of FCR was detectable in excised roots and was stimulated about 20_times in C. junos and only about 3_times in P. trifoliata under iron deficiency for four weeks. The FRO2 of Arabidopsis was used as a probe, the tissue print technique was used to ascertain the expression of the FCR gene in C. junos and P. trifoliata under iron stress. High_level transcripts were observed in the absorptive root, young green stem as well as new leaf of C. junos under iron stress for two weeks, and the transcripts were accumulated only slightly in P. trifoliata at the same time. The results showed that the obvious increase of FCR activity was an important reason for the tolerance of C. junos to iron_deficiency, and the regulation of FCR activity seemed to be at the transcriptional level, and the expression of FRO2 occurred in the root, stem and leaf. 展开更多
关键词 Citrus junos Poncirus trifoliata iron stress ferric chelate_reductase tissue print FRO2 gene Northern hybridization
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基于JUNO卫星WAVES仪器波动数据的木星磁层哨声波分析研究 被引量:2
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作者 黄靖 倪彬彬 +8 位作者 付松 顾旭东 曹兴 项正 王琦 罗琼 何颖 闫玲 王敬之 《地球物理学报》 SCIE EI CAS CSCD 北大核心 2019年第3期817-824,共8页
等离子体波的空间分布在木星磁层高能电子动力学过程中起着重要的作用.现有大多数对木星磁层哨声波的观测仅限于|λ|≤15°的磁纬范围内,但是最新的JUNO卫星WAVES仪器提供的波动数据使得更高纬度、更广区域范围内的等离子体波动分... 等离子体波的空间分布在木星磁层高能电子动力学过程中起着重要的作用.现有大多数对木星磁层哨声波的观测仅限于|λ|≤15°的磁纬范围内,但是最新的JUNO卫星WAVES仪器提供的波动数据使得更高纬度、更广区域范围内的等离子体波动分布研究成为可能.本文通过对JUNO卫星WAVES仪器数据进行分析处理,详细研究了木星磁层哨声波的空间分布特性.观测表明,存在位于高LJ、高磁纬的木星磁层哨声波,它们广泛分布于距木星中心距离35~75个木星半径、磁纬为|λ|≤30°的空间区域.分析研究发现,WAVES仪器观测的木星磁层哨声波幅度一般为几个pT,远小于地球磁层哨声波的强度.木星磁层哨声波幅会随着LJ的增大缓慢增加,也会随着磁纬的减小趋向平缓变化.基于以上观测事实,本文利用指数幂函数分别拟合得到木星磁层哨声波幅随LJ和磁纬变化的经验模型.该模型将有助于精确理解哨声波对木星磁层高能电子动力学过程的重要影响. 展开更多
关键词 木星磁层 juno卫星 哨声波 统计分析
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哺乳动物精卵融合必需蛋白质IZUMO1-JUNO/CD9的研究进展 被引量:1
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作者 张英楠 黄佳星 +3 位作者 梁欣然 李芽 于书海 王郑 《生命科学研究》 CAS CSCD 2019年第3期226-230,共5页
精卵融合是受精过程中最为重要的步骤。目前公认IZUMO1、JUNO和CD9(cluster of differentiation antigen 9)为精卵融合的必需蛋白质,其中IZUMO1与JUNO在精卵识别时会形成复合体。有研究表明IZUMO1、JUNO和CD9主要参与精卵融合最初的黏... 精卵融合是受精过程中最为重要的步骤。目前公认IZUMO1、JUNO和CD9(cluster of differentiation antigen 9)为精卵融合的必需蛋白质,其中IZUMO1与JUNO在精卵识别时会形成复合体。有研究表明IZUMO1、JUNO和CD9主要参与精卵融合最初的黏附过程,且它们之间是相互关联发挥作用的。近年来由于X射线晶体学相关技术的发展,IZUMO1-JUNO晶体结构基本被阐明,然而精卵融合的具体分子机制仍未被完全揭示。所以,对哺乳动物精卵融合必需蛋白质IZUMO1-JUNO/CD9的结构、功能和分子机制进行阐述是十分必要的。 展开更多
关键词 精卵融合 IZUMO1蛋白 juno蛋白 CD9蛋白
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Expression,structure and function analysis of the sperm-oocyte fusion genes Juno and Izumo1 in sheep(Ovis aries) 被引量:3
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作者 Wenping Hu Xinlong Dong +5 位作者 Zhilong Tian Zhuangbiao Zhang Jishun Tang Benmeng Liang Qiuyue Liu Mingxing Chu 《Journal of Animal Science and Biotechnology》 SCIE CAS CSCD 2021年第3期917-934,共18页
Background:JUNO and IZUMO1 are the first receptor-ligand protein pairs discovered to be essential for spermoocyte fusion;their interaction is indispensable for fertilization.Methods:PCR was used to clone the full-leng... Background:JUNO and IZUMO1 are the first receptor-ligand protein pairs discovered to be essential for spermoocyte fusion;their interaction is indispensable for fertilization.Methods:PCR was used to clone the full-length DNA sequence of the Juno gene in sheep.The single nucleotide polymorphism(SNP)loci of Juno were genotyped by Sequenom MassARRAY®.PCR combined with rapid amplification of cDNA Ends were used to clone the full-length cDNA sequence of Juno and Izumo1.Reverse transcriptase-PCR(RT-PCR)and real time-quantitative-PCR(RT-qPCR)were used to analyze the genes’expression in tissues of sheep,and single cell RNA-seq was used to analyze the genes’expression in oocytes,granulosa cells and follicular theca of polytocous and monotocous Small Tail Han ewes.Bioinformatics was used to analyze advanced structure and phylogeny of JUNO and IZUMO1 proteins.Results:The full-length DNA sequence of the Juno gene in sheep was cloned and nine SNPs were screened.We found a significant association between the g.848253 C>A locus of Juno and litter size of Small Tail Han sheep(P<0.05).The full-length cDNA sequence of Juno and Izumo1 genes from Small Tail Han sheep were obtained.We found a new segment of the Izumo1 CDS consisting of 35 bp,and we confirmed the Izumo1 gene has 9 exons,not 8.RT-qPCR showed that Juno and Izumo1 genes were highly expressed in ovarian and testicular tissues,respectively(P<0.01).Single cell RNA-seq showed Juno was specifically expressed in oocytes,but not in granulosa cells or follicular theca,while Izumo1 displayed little to no expression in all three cell types.There was no difference in expression of the Juno gene in oocyte and ovarian tissue in sheep with different litter sizes,indicating expression of Juno is not related to litter size traits.Bioinformatic analysis revealed the g.848253 C>A locus of Juno results in a nonconservative missense point mutation leading to a change from Phe to Leu at position 219 in the amino acid sequence.Conclusions:For the first time,this study systematically analyzed the expression,structure and function of Juno and Izumo1 genes and their encoded proteins in Small Tail Han sheep,providing the basis for future studies of the regulatory mechanisms of Juno and Izumo1 genes. 展开更多
关键词 FERTILIZATION Izumo1 juno SHEEP Single cell RNA-seq
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江门中微子实验(JUNO)中心探测器结构在浮力下的整体稳定性研究 被引量:1
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作者 李华峰 《建筑结构》 CSCD 北大核心 2021年第20期76-81,共6页
介绍了江门中微子实验(JUNO)中心探测器主体不锈钢结构的结构体系,阐述了结构在巨大浮力作用下的整体稳定性问题及失稳模式,并针对结构的特点提出了结构整体稳定性评价标准。通过对一系列模型的稳定性分析和对比发现结构主要的失稳形式... 介绍了江门中微子实验(JUNO)中心探测器主体不锈钢结构的结构体系,阐述了结构在巨大浮力作用下的整体稳定性问题及失稳模式,并针对结构的特点提出了结构整体稳定性评价标准。通过对一系列模型的稳定性分析和对比发现结构主要的失稳形式是有机玻璃球在浮力作用下的整体旋转上升。与不锈钢网壳刚接的撑杆的数目和位置是影响结构整体稳定性的重要因素。所有撑杆两端均铰接的方案存在提前失稳的风险。有机玻璃球的初始整体旋转、撑杆与有机玻璃球表面不完全垂直等初始缺陷会一定程度上削弱结构的整体稳定性。随着撑杆随机偏转角标准差的增加,结构整体稳定性呈缓慢降低的趋势。根据分析结果,结构考虑初始缺陷的双非线性稳定承载力系数可取3.35,满足设计要求。 展开更多
关键词 江门中微子实验 有机玻璃球 不锈钢 单层网壳 稳定性 浮力 初始缺陷
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Trimble JUNO SB在森林资源连续清查中的应用
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作者 张晓星 谢锋珠 《林业实用技术》 北大核心 2011年第9期68-70,共3页
通过对Trimble Juno SB GPS的坐标系统的设置,导航点与背景文件的制作,结合"连清"工作的具体实例,研究和探讨了Juno SB在森林资源连续清查中应用的主要应用时的优点和存在的问题。
关键词 TRIMBLE juno SB GPS森林资源连续清查
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Afterpulse measurement of JUNO 20‑inch PMTs
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作者 Rong Zhao Nikolay Anfimov +13 位作者 Yu Chen Hang Hu Jun Hu Xiao‑Lu Ji Denis Korablev Min Li Alexander Olshevskiy Zhao‑Yuan Peng Arseny Rybnikov Zhong‑Hua Qin Jun Wang Wei Wang Zhi‑Min Wang Björn Wonsak 《Nuclear Science and Techniques》 SCIE EI CAS CSCD 2023年第1期136-145,共10页
In this study,we present the large photomultiplier tube(PMT)afterpulse measurement results obtained from the Jiangmen underground neutrino observatory(JUNO)experiment.A total of 11 dynode-PMTs(R12860)from the Hamamats... In this study,we present the large photomultiplier tube(PMT)afterpulse measurement results obtained from the Jiangmen underground neutrino observatory(JUNO)experiment.A total of 11 dynode-PMTs(R12860)from the Hamamatsu company(Hamamatsu Photonics K.K.(HPK))and 150 micro-channel plate PMTs(MCP-PMTs,GDB-6201)from the NNVT company(North Night Vision Technology Co.,Ltd.(NNVT))were tested.Subsequently,an afterpulse model was built according to the afterpulse time distribution and the probability of occurrence for these two types of PMTs.The average ratio of the total afterpulse charge with a delay between 0.5μs and 20μs to the primary pulse charge is∼5.7%(13.2%)for the tested MCPPMTs(dynode-PMTs).The JUNO experiment will deploy 20,01220-inch PMTs;this study will benefit detector simulation,event reconstruction,and data analysis regarding the JUNO experiment. 展开更多
关键词 Afterpulse MCP-PMT juno Dynode-PMT 20-inch PMT
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Reconstruction of a muon bundle in the JUNO central detector
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作者 Cheng-Feng Yang Yong-Bo Huang +6 位作者 Ji-Lei Xu Di-Ru Wu Yong-Peng Zhang Wu-Ming Luo Miao He Guo-Ming Chen Si-Yuan Zhang 《Nuclear Science and Techniques》 SCIE EI CAS CSCD 2022年第5期78-90,共13页
The Jiangmen Underground Neutrino Observatory(JUNO)is a multi-purpose neutrino experiment.One of the main goals is to determine the neutrino mass ordering by precisely measuring the energy spectrum of reactor antineut... The Jiangmen Underground Neutrino Observatory(JUNO)is a multi-purpose neutrino experiment.One of the main goals is to determine the neutrino mass ordering by precisely measuring the energy spectrum of reactor antineutrinos.For the detection of reactor antineutrinos,cosmogenic backgrounds,such as^(9)Li/^(8)He and fast neutrons induced by cosmic muons,should be rejected carefully by applying muon veto cuts,which require good muon track reconstruction.With a 20-kton liquid scintillator detector,the simulation shows the proportion of muon bundles(muon multiplicity≥2)to be approximately 8%in JUNO,whereas its reconstruction has been rarely discussed in previous experiments.This study proposes an efficient algorithm for muon track reconstruction based on the charge response of a photomultiplier tube array.This is the first reconstruction of muon bundles in a large-volume liquid scintillator detector.In addition,the algorithm shows good performance and potential for reconstruction for both a single muon and double muons(muon multiplicity=2).The spatial resolution of a single-muon reconstruction was20 cm,and the angular resolution was 0.5°.For doublemuon reconstruction,the spatial and angular resolutions could be 30 cm and 1.0°,respectively.Moreover,this paper also discusses muon classification and the veto strategy. 展开更多
关键词 juno Liquid scintillatordetector Muon reconstruction Muon bundle Veto strategy
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Pain-Relief Effects of Aroma Touch Therapy with <i>Citrus junos</i>Oil Evaluated by Quantitative EEG Occipital Alpha-2 Rhythm Powers
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作者 Tomomi Bohgaki Yoshitada Katagiri Makoto Usami 《Journal of Behavioral and Brain Science》 2014年第1期11-22,共12页
Aroma touch therapy is widely used in clinical fields for alleviating pain-related symptoms;however, few studies have reported the pain-relief mechanisms. The present study aimed to elucidate the analgesic effects of ... Aroma touch therapy is widely used in clinical fields for alleviating pain-related symptoms;however, few studies have reported the pain-relief mechanisms. The present study aimed to elucidate the analgesic effects of aroma touch therapy with Citrus junos oil based on the quantitative evaluation of deep brain network (DBN) activity using electroencephalogram (EEG) occipital alpha-2 rhythm (10-13 Hz) powers. Experimental investigations were performed with 13 healthy volunteers using the cold pressor task for simulating chronic pain in three different sessions: a baseline session with no therapies, a control session with a touch therapy, and an aroma touch therapy. We have found for the first time that the interviewed pain ratings represented by Numeric Rating Scale (NRS) scores were strongly correlated with a DBN activity index, which was derived from the slow fluctuation components of occipital EEG alpha-2 rhythm powers. The correlation was characterized by a V-shaped curve in the DBN activity index versus the pain rating, i.e., the NRS score, which provided the complete analgesic states (NRS = 0) for some subjects under aroma touch therapy at an appropriate DBN activity index. Such analgesic states were not so strongly correlated with emotional valence. In conclusion, aroma touch therapy may directly modulate DBN activity so that pain-induced outcomes are minimized. 展开更多
关键词 AROMA TOUCH THERAPY Chronic Pain Encephalogram OCCIPITAL Alpha-2 RHYTHM Citrus junos (Yuzu) OIL
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Anatomical Structure of Aboveground and Underground Organs of the Rare Endemic Species <i>Iris (Juno) magnifica</i>vved., Growing under Natural Conditions of the Zeravshan Ridge, Samarkand Mountains
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作者 Nargiza K. Rakhimova Guljan M. Duschanova +1 位作者 Akida T. Abdullaeva Eldor E. Temirov 《American Journal of Plant Sciences》 2020年第9期1453-1466,共14页
The morpho-anatomical structure of the aboveground and underground organs of the rare endemic species </span><i><span style="font-family:Verdana;">Iris </span></i><span style... The morpho-anatomical structure of the aboveground and underground organs of the rare endemic species </span><i><span style="font-family:Verdana;">Iris </span></i><span style="font-family:Verdana;">(</span><i><span style="font-family:Verdana;">Juno</span></i><span style="font-family:Verdana;">)</span><i> <span style="font-family:Verdana;">magnifica</span></i><span style="font-family:Verdana;">, growing under natural conditions of the Zeravshan ridge, Samarkand mountains, has been studied for the first time. A comparative analysis of the morpho-anatomical structure of the aboveground and underground organs revealed characteristic diagnostic signs of a microscopic structure. The complex of anatomical features of the aboveground and underground organs of the studied species are species-specific and can be used to solve taxonomic problems of this genus of plants, as well as the Red Book endemic species of </span><span style="font-family:Verdana;">juno</span><span style="font-family:Verdana;"> irises, are of particular interest in connection with the potential for their vegetative reproduction. 展开更多
关键词 Anatomy Aboveground and Underground Organs Iris (juno) magnifica Zeravshan Ridge Samarkand Mountains
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The Study of the Psychic Remnants in Juno and the Paycock
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作者 Hafsah Zafr 《Journal of Literature and Art Studies》 2017年第8期1012-1019,共8页
This article involves the study of the psychic remnants commonly known as Archetypes in Sean O'Casey's play Juno and the Paycock. Archetypes are the images or patterns recurring again and again in literature through... This article involves the study of the psychic remnants commonly known as Archetypes in Sean O'Casey's play Juno and the Paycock. Archetypes are the images or patterns recurring again and again in literature through the ages. It also focuses on the minute difference between archetype and archetypal image as discussed by Jung with special reference to the characters and other images in the play beating relevance with the universal archetypes. This article also highlights the play as a connective link in the series of the different pieces of literature via the unique use of the psychic remnants. It emphasises on the different use of those remnants interwoven in the mosaic of the characters and plot of the play. 展开更多
关键词 ARCHETYPES archetypal image JUNG universal archetypes juno and the Paycock
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木星探测器Juno精密定轨分析及低阶引力场解算 被引量:1
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作者 秦松鹤 黄勇 +1 位作者 李培佳 曹建峰 《武汉大学学报(信息科学版)》 EI CAS CSCD 北大核心 2023年第1期65-74,共10页
随着中国深空测控技术的进步和深空探测计划的推进,木星探测计划已经进入日程,木星探测器的精密定轨和木星的引力场的解算是木星探测中的重要研究内容。首先给出了木星探测器的坐标系统和动力学模型,并利用已公布的朱诺号木星探测器精... 随着中国深空测控技术的进步和深空探测计划的推进,木星探测计划已经进入日程,木星探测器的精密定轨和木星的引力场的解算是木星探测中的重要研究内容。首先给出了木星探测器的坐标系统和动力学模型,并利用已公布的朱诺号木星探测器精密星历数据进行验证,动力学拟合结果与参考星历的位置偏差在10 m量级,速度偏差小于6 mm/s;然后利用深空多普勒测量模型处理已经发布的朱诺号无线电测量数据进行精密定轨,结果与参考星历的差距在数百米量级;最后利用仿真数据验证引力场系数解算的可靠性,并利用朱诺号探测器4个近木点附近的实测数据解算引力场系数,得到了截至8阶的带谐项系数。 展开更多
关键词 精密定轨 朱诺号探测器 木星引力场
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应用于JUNO实验的容器技术研究
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作者 谭宏楠 石京燕 +3 位作者 邹佳恒 杜然 姜晓巍 孙震宇 《计算机工程》 CAS CSCD 北大核心 2019年第4期1-5,共5页
江门中微子实验(JUNO)是以测定中微子质量顺序、精确测量中微子混合参数为主要目的的一项物理科学前沿研究实验,其实验规模庞大,数据处理流程繁杂,需借助统一高效的离线计算平台对数据进行分析处理。为此,利用Docker容器分层的镜像技术... 江门中微子实验(JUNO)是以测定中微子质量顺序、精确测量中微子混合参数为主要目的的一项物理科学前沿研究实验,其实验规模庞大,数据处理流程繁杂,需借助统一高效的离线计算平台对数据进行分析处理。为此,利用Docker容器分层的镜像技术将JUNO实验所需的环境依赖库打包在镜像文件中,为其制定针对不同操作系统作业的容器镜像,并将不同JUNO容器作业提交至作业调度器上运行,以实现资源共享。对物理机、容器、虚拟机3种平台的CPU性能、I/O性能及JUNO作业的实际运行效果进行对比测试,结果表明,Docker容器能够胜任JUNO离线数据处理,相比虚拟机具有更小的性能损耗。 展开更多
关键词 虚拟机 Docker容器 镜像 江门中微子实验 虚拟化技术
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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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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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JUNO Formally Comes into Operation
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作者 SONG Jianlan 《Bulletin of the Chinese Academy of Sciences》 2025年第3期145-148,共4页
This colossal instrument is set to determine the mass ordering of neutrinos-whether or not one type of neutrinos is heavier than another,and more.
关键词 neutrino mass ordering determine mass ordering juno
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