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基于嗅觉可视化技术的眉茶等级分类方法 被引量:1
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作者 丁煜函 葛东营 +2 位作者 荆磊 muhammad shahzad 江辉 《食品科学》 EI CAS CSCD 北大核心 2022年第24期335-341,共7页
为了快速、准确地对眉茶等级进行分类,提出了一种基于嗅觉可视化技术的眉茶等级快速分类方法。首先,根据卟啉显色反应预实验结果,选定了12种显色效果明显的卟啉指示剂制备嗅觉可视化传感器阵列,通过该传感器阵列与不同等级的眉茶茶汤进... 为了快速、准确地对眉茶等级进行分类,提出了一种基于嗅觉可视化技术的眉茶等级快速分类方法。首先,根据卟啉显色反应预实验结果,选定了12种显色效果明显的卟啉指示剂制备嗅觉可视化传感器阵列,通过该传感器阵列与不同等级的眉茶茶汤进行反应,获取不同的特征图像。然后,对特征图像数据进行主成分分析和降维,将得到的不同维数的主成分分析结果作为输入变量,构建支持向量机(support vector machine,SVM)眉茶等级分类模型。最后,引入3种群体智能优化算法(萤火虫算法、灰狼优化算法、布谷鸟算法)对SVM分类模型的惩罚因子c和核函数参数g进行优化。结果显示:未经优化的SVM分类模型对测试集的分类正确率为80%,所需的主成分个数为12个;经过优化的SVM模型的分类正确率均有所提升,其中经过布谷鸟算法优化的SVM模型对测试集的分类正确率达到了93.3%,且所需的主成分个数减少为6个。这表明应用嗅觉可视化技术能够实现对眉茶等级的分类,而通过群体智能优化算法优化SVM分类模型可以显著增强模型的性能,提高分类正确率。 展开更多
关键词 眉茶 嗅觉可视化 等级分类 支持向量机 群体智能优化算法
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利用抑制性消减杂交技术筛选大鼠哮喘相关基因
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作者 钟波 王慧莲 +5 位作者 muhammad shahzad 宁启兰 韩燕 杨旭东 张富军 吕社民 《浙江大学学报(医学版)》 CAS CSCD 北大核心 2009年第4期362-369,共8页
目的:利用哮喘大鼠模型筛选与哮喘发病相关的差异性表达基因。方法:采用抑制性消减杂交技术,以哮喘大鼠肺组织总RNA为检验子,对照大鼠肺组织总RNA为驱赶子,将消减杂交获得的DNA片断与pGEM-T Easy Vector连接,构建cDNA文库后,转化大肠杆... 目的:利用哮喘大鼠模型筛选与哮喘发病相关的差异性表达基因。方法:采用抑制性消减杂交技术,以哮喘大鼠肺组织总RNA为检验子,对照大鼠肺组织总RNA为驱赶子,将消减杂交获得的DNA片断与pGEM-T Easy Vector连接,构建cDNA文库后,转化大肠杆菌DH5α,筛选阳性克隆。将获得的阳性克隆插入片段进行测序分析,测序结果与GenBank数据库中cDNA和EST序列进行相似性比对,获得差异性表达基因的信息。结果:扩增消减cDNA文库获得300余个白色克隆,随即挑选36个测序,除去重复序列,结果中含有已知的基因4个,ESTs 2个及与任何序列无同源性的新基因片段3个。结论:成功构建了哮喘大鼠肺脏差异性表达基因的正向消减cDNA文库,筛选出数个与哮喘相关的差异表达基因。 展开更多
关键词 哮喘/免疫学 哮喘/病理生理学 抑制性消减杂交 差异性表达基因 CDNA文库
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STEMI患者PCI术后左心室GLS、梗死面积变化及与主要不良心血管事件的关系 被引量:5
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作者 段洋 陆远 +5 位作者 王志荣 徐晤 李承宗 王晓萍 韩曙光 muhammad shahzad 《山东医药》 CAS 北大核心 2017年第27期99-101,共3页
目的观察急性ST段抬高型心肌梗死(STEMI)患者介入治疗(PCI)后6个月左心室整体纵向应变(GLS)及心肌梗死面积(IS)的变化,并探讨二者与PCI术后6~12个月主要不良心血管事件(MACE)发生情况的关系。方法选择60例PCI术后STEMI患者(其中7例PCI术... 目的观察急性ST段抬高型心肌梗死(STEMI)患者介入治疗(PCI)后6个月左心室整体纵向应变(GLS)及心肌梗死面积(IS)的变化,并探讨二者与PCI术后6~12个月主要不良心血管事件(MACE)发生情况的关系。方法选择60例PCI术后STEMI患者(其中7例PCI术后6~12个月发生MACE)。PCI术后7 d、6个月分别采用二维超声心动图斑点追踪成像技术测算左心室GLS,采用延迟增强心磁共振技术测算左心室IS。结果本组患者PCI术后7 d、6个月左心室GLS分别为-14%±3%、-17%±3%,IS分别为23%±7%、19%±6%。本组患者PCI术后6个月左心室GLS、IS均低于术后7 d,P均<0.05。相关性分析显示,本组患者PCI术后左心室GLS和IS呈负相关(r=-0.756,P<0.01)。本组患者PCI术后6个月左心室GLS较术后7 d降低2%~4%,中位数为3%。以PCI术后6个月左心室GLS较术后7 d降低幅度的中位数为界值将本组患者分为GLS明显降低组(降低幅度≥中位数)26例和GLS无明显降低组(降低幅度<中位数)34例,其中分别有0、7例患者随访过程中发生MACE,两组MACE发生率相比,P<0.05。本组患者PCI术后6个月IS较术后7 d降低2%~5%,中位数为3%。以PCI术后6个月IS较术后7 d降低幅度的中位数为界值将本组患者分为IS明显降低组(降低幅度≥中位数)21例和IS无明显降低组(降低幅度<中位数)39例,其中分别有0、7例患者随访过程中发生MACE,两组MACE发生率相比,P<0.05。结论 STEMI患者PCI术后6个月左心室GLS和IS低于术后7 d;STEMI患者PCI术后左心室GLS、IS有较好的相关性;STEMI患者PCI术后左心室GLS、IS明显降低者不易发生MACE。 展开更多
关键词 心肌梗死 梗死面积 纵向应变 主要不良心血管事件
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黄连素对福美双诱导的肉鸡胫骨软骨发育不良的影响 被引量:2
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作者 王智 张鼎 +4 位作者 李坤 刘晶英 韩照清 muhammad shahzad 李家奎 《中国兽医学报》 CAS CSCD 北大核心 2015年第12期2037-2040,共4页
为探讨黄连素(berberin)通过调控基质金属蛋白酶诱导因子(EMMPRIN)又名CD147的表达对肉鸡胫骨软骨发育不良(TD)的影响,将150只1日龄AA肉鸡随机均分为3组:对照组、TD发生组和黄连素组,对照组正常饲喂基础日粮;从第3天开始,TD发生组和黄... 为探讨黄连素(berberin)通过调控基质金属蛋白酶诱导因子(EMMPRIN)又名CD147的表达对肉鸡胫骨软骨发育不良(TD)的影响,将150只1日龄AA肉鸡随机均分为3组:对照组、TD发生组和黄连素组,对照组正常饲喂基础日粮;从第3天开始,TD发生组和黄连素组,在饲喂基础日粮的同时添加25 mg/kg的福美双诱导产生TD,黄连素组从第7天开始口腔灌服黄连素,剂量为15 mg/kg,连用7 d。于第14天剖杀全部雏鸡。观察记录各组雏鸡体质量变化、HE染色观察生长板结构及血管变化,real-time PCR和Western blot检测CD147基因和蛋白的表达差异。结果显示,TD发生组雏鸡体质量增长缓慢,生长板组织结构破坏严重,且CD147基因及蛋白表达量显著下降。黄连素组雏鸡体质量增长较快,TD症状缓解,生长板血管浸润较多,且CD147基因及蛋白表达量增加。由此推测,饲料中添加黄连素可以上调CD147基因和蛋白的表达量,从而促进TD病变区血管的生成和恢复,缓解TD症状,提高肉鸡产量。 展开更多
关键词 黄连素 福美双 肉鸡 胫骨软骨发育不良 基质金属蛋白酶诱导因子
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表没食子儿茶素没食子酸酯对福美双诱导的肉鸡胫骨软骨发育不良的影响
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作者 刘晶英 张鼎 +4 位作者 李坤 王智 韩照清 muhammad shahzad 李家奎 《中国兽医学报》 CAS CSCD 北大核心 2015年第8期1334-1338,共5页
旨在研究表没食子儿茶素没食子酸酯(EGCG)通过调控热休克蛋白HSP90的表达对肉鸡胫骨软骨发育不良(TD)的影响。试验将120羽1日龄健康AA肉鸡预饲1周后随机分成3组:对照组、TD发生组和EGCG处理组。通过向基础日粮中添加药物的方式,分别对T... 旨在研究表没食子儿茶素没食子酸酯(EGCG)通过调控热休克蛋白HSP90的表达对肉鸡胫骨软骨发育不良(TD)的影响。试验将120羽1日龄健康AA肉鸡预饲1周后随机分成3组:对照组、TD发生组和EGCG处理组。通过向基础日粮中添加药物的方式,分别对TD发生组和EGCG处理组雏鸡饲喂25mg/kg的福美双,诱发TD。从第3日起,对EGCG处理组雏鸡每天腹腔注射10mg/kg的EGCG。14d后,全部扑杀试验鸡。形态学检查肉鸡胫骨生长板发育状况;HE染色法观察生长板软骨细胞分化和血管生成变化;Real-time PCR和Western blot法分别检测HSP90基因和蛋白表达差异。结果显示,TD发生组雏鸡TD症状明显,HSP90基因和蛋白表达量均明显上升。EGCG处理组雏鸡TD症状明显缓解,HSP90基因和蛋白表达量显著下降;生长板软骨细胞分化和血管浸润显著恢复。由此推测,EGCG可能通过下调HSP90基因和蛋白在TD肉鸡软骨细胞中的表达,恢复TD胫骨病变区软骨细胞分化和血管生成,抑制TD发生,提高肉鸡健康状况。 展开更多
关键词 儿茶素 福美双 肉鸡 胫骨软骨发育不良 热休克蛋白
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Effect of Firing Temperature on the Electromagnetic Properties of Electronic Transformer Cores Developed by Using Nanosized Mn–Zn Ferrite Powders 被引量:2
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作者 Hassan Waqas Ammad Hussain Qureshi muhammad shahzad 《Acta Metallurgica Sinica(English Letters)》 SCIE EI CAS CSCD 2015年第2期159-163,共5页
Current investigation deals with the effect of grain growth process as a function of sintering temperature on the electromagnetic properties (initial permeability, impedance, and gain) of Mn-Zn ferrite (MZF) cores... Current investigation deals with the effect of grain growth process as a function of sintering temperature on the electromagnetic properties (initial permeability, impedance, and gain) of Mn-Zn ferrite (MZF) cores (toroids). By employing auto combustion process, nanosized [(20 ± 5) nm] MZF powders were synthesized and toroid shape cores were obtained after subsequent calcination and firing (sintering) process. It was observed that the submicron structure (0.5 μm) achieved in the ferrite core sintered at 1,000 ℃ was gradually transformed into micron size grains by increasing the firing temperature i.e., 1,100, 1,200, and 1,350 ℃. The results reveal that MZF core sintered at low temperature (1,000 ℃) showed high impedance, low initial permeability, and narrow working frequency range i.e., 3-15 MHz. However, the improvement in initial permeability, sintered density, and operational frequency range (100 kHz-17 MHz) was observed at high temperature (1,350 ℃) firing in the inert environment. This synthesized MZF core is more suitable for miniaturized switch mode power supply applications. 展开更多
关键词 Mn-Zn ferrites Nanosized powders IMPEDANCE SINTERING
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Feasibility and physics potential of detecting ^(8)B solar neutrinos at JUNO 被引量:1
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作者 Angel Abusleme Thomas Adam +590 位作者 Shakeel Ahmad Sebastiano Aiello muhammad Akram Nawab Ali Fengpeng An Guangpeng An Qi An Giuseppe Andronico Nikolay Anfimov Vito Antonelli Tatiana Antoshkina Burin Asavapibhop João Pedro Athayde Marcondes de André Didier Auguste Andrej Babic Wander Baldini Andrea Barresi Eric Baussan Marco Bellato Antonio Bergnoli Enrico Bernieri David Biare Thilo Birkenfeld Sylvie Blin David Blum Simon Blyth Anastasia Bolshakova Mathieu Bongrand Clément Bordereau Dominique Breton Augusto Brigatti Riccardo Brugnera Riccardo Bruno Antonio Budano Max Buesken Mario Buscemi Jose Busto Ilya Butorov Anatael Cabrera Hao Cai Xiao Cai Yanke Cai Zhiyan Cai 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 Shenjian Chen Xurong Chen Yi-Wen Chen Yixue Chen Yu Chen Zhang Chen Jie Cheng Yaping Cheng Alexander Chepurnov Davide Chiesa Pietro Chimenti Artem Chukanov Anna Chuvashova Gérard Claverie Catia Clementi Barbara Clerbaux Selma Conforti Di Lorenzo Daniele Corti Salvatore Costa Flavio Dal Corso Christophe De La Taille Jiawei Deng Zhi Deng Ziyan Deng Wilfried Depnering Marco Diaz Xuefeng Ding Yayun Ding Bayu Dirgantara Sergey Dmitrievsky Tadeas Dohnal Georgy Donchenko Jianmeng Dong Damien Dornic Evgeny Doroshkevich Marcos Dracos Frédéric Druillole Shuxian Du Stefano Dusini Martin Dvorak Timo Enqvist Heike Enzmann Andrea Fabbri Lukas Fajt Donghua Fan Lei Fan Can Fang Jian Fang Marco Fargetta Anna Fatkina Dmitry Fedoseev Vladko Fekete Li-Cheng Feng Qichun Feng Richard Ford Andrey Formozov Amélie Fournier Haonan Gan Feng Gao Alberto Garfagnini Alexandre Göttel Christoph Genster Marco Giammarchi Agnese Giaz Nunzio Giudice Franco Giuliani Maxim Gonchar Guanghua Gong Hui Gong Oleg Gorchakov Yuri Gornushkin Marco Grassi Christian Grewing Maxim Gromov 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 Miao He Wei He Tobias Heinz Patrick Hellmuth Yuekun Heng Rafael Herrera Daojin Hong YuenKeung Hor Shaojing Hou Yee Hsiung Bei-Zhen Hu Hang Hu Jianrun Hu Jun Hu Shouyang Hu Tao Hu Zhuojun Hu Chunhao Huang Guihong Huang Hanxiong Huang Qinhua Huang Wenhao Huang Xingtao Huang Yongbo Huang Jiaqi Hui Wenju Huo Cédric Huss Safeer Hussain Antonio Insolia Ara Ioannisian Daniel Ioannisyan Roberto Isocrate Kuo-Lun Jen Xiaolu Ji Xingzhao Ji Huihui Jia Junji Jia Siyu Jian Di Jiang Xiaoshan Jiang Ruyi Jin Xiaoping Jing Cécile Jollet Jari Joutsenvaara Sirichok Jungthawan Leonidas Kalousis Philipp Kampmann Li Kang Michael Karagounis Narine Kazarian Amir Khan Waseem Khan Khanchai Khosonthongkee Patrick Kinz Denis Korablev Konstantin Kouzakov Alexey Krasnoperov Svetlana Krokhaleva Zinovy Krumshteyn Andre Kruth Nikolay Kutovskiy Pasi Kuusiniemi Tobias Lachenmaier Cecilia Landini Sébastien Leblanc Frederic Lefevre Liping Lei Ruiting Lei Rupert Leitner Jason Leung Demin Li Fei Li Fule Li Haitao Li Huiling Li Jiaqi Li Jin Li Kaijie Li Mengzhao Li Nan Li Nan Li Qingjiang Li Ruhui Li Shanfeng Li Shuaijie Li Tao Li Weidong Li Weiguo Li Xiaomei Li Xiaonan Li Xinglong Li Yi Li Yufeng Li Zhibing Li Ziyuan Li Hao Liang Hao Liang Jingjing 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 Hu Liu Hui Liu Jianglai Liu Jinchang Liu Min Liu Qian Liu Qin Liu Runxuan Liu Shuangyu Liu Shubin Liu Shulin Liu Xiaowei Liu Yan 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 Fengjiao Luo Guang Luo Pengwei Luo Shu Luo Wuming Luo Vladimir Lyashuk Qiumei Ma Si Ma Xiaoyan Ma Xubo Ma Jihane Maalmi Yury Malyshkin Fabio Mantovani Francesco Manzali Xin Mao Yajun Mao Stefano MMari Filippo Marini Sadia Marium Cristina Martellini Gisele Martin-Chassard Agnese Martini Davit Mayilyan Axel Müller Ints Mednieks Yue Meng Anselmo Meregaglia Emanuela Meroni David Meyhöfer Mauro Mezzetto Jonathan Miller Lino Miramonti Salvatore Monforte Paolo Montini Michele Montuschi Nikolay Morozov Pavithra Muralidharan Massimiliano Nastasi Dmitry VNaumov Elena Naumova Igor Nemchenok Alexey Nikolaev Feipeng Ning Zhe Ning Hiroshi Nunokawa Lothar Oberauer Juan Pedro Ochoa-Ricoux Alexander Olshevskiy Domizia Orestano Fausto Ortica Hsiao-Ru Pan Alessandro Paoloni Nina Parkalian Sergio Parmeggiano Teerapat Payupol Yatian Pei Nicomede Pelliccia Anguo Peng Haiping Peng Frédéric Perrot Pierre-Alexandre Petitjean Fabrizio Petrucci Luis Felipe Piñeres Rico Oliver Pilarczyk Artyom Popov Pascal Poussot Wathan Pratumwan Ezio Previtali Fazhi Qi Ming Qi Sen Qian Xiaohui Qian Hao Qiao Zhonghua Qin Shoukang Qiu muhammad Rajput Gioacchino Ranucci Neill Raper Alessandra Re Henning Rebber Abdel Rebii Bin Ren Jie Ren Taras Rezinko Barbara Ricci Markus Robens Mathieu Roche Narongkiat Rodphai Aldo Romani Bedřich Roskovec Christian Roth Xiangdong Ruan Xichao Ruan Saroj Rujirawat Arseniy Rybnikov Andrey Sadovsky Paolo Saggese Giuseppe Salamanna Simone Sanfilippo Anut Sangka Nuanwan Sanguansak Utane Sawangwit Julia Sawatzki Fatma Sawy Michaela Schever Jacky Schuler Cédric Schwab Konstantin Schweizer Dmitry Selivanov Alexandr Selyunin Andrea Serafini Giulio Settanta Mariangela Settimo muhammad shahzad Vladislav Sharov Gang Shi Jingyan Shi Yongjiu Shi Vitaly Shutov Andrey Sidorenkov FedorŠimkovic Chiara Sirignano Jaruchit Siripak Monica Sisti Maciej Slupecki Mikhail Smirnov Oleg Smirnov Thiago Sogo-Bezerra Julanan Songwadhana Boonrucksar Soonthornthum Albert Sotnikov Ondrej Sramek Warintorn Sreethawong Achim Stahl Luca Stanco Konstantin Stankevich DušanŠtefánik Hans Steiger Jochen Steinmann Tobias Sterr Matthias Raphael Stock Virginia Strati Alexander Studenikin Gongxing Sun 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 Konstantin Treskov Andrea Triossi Giancarlo Troni Wladyslaw Trzaska Cristina Tuve Stefan van Waasen Johannes van den Boom Guillaume Vanroyen Nikolaos Vassilopoulos Vadim Vedin Giuseppe Verde Maxim Vialkov Benoit Viaud Cristina Volpe Vit Vorobel 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 Ruiguang Wang Siguang Wang Wei Wang Wenshuai Wang Xi Wang Xiangyue Wang Yangfu Wang Yaoguang Wang Yi Wang Yifang Wang Yuanqing Wang Yuman Wang Zhe Wang Zheng Wang Zhimin Wang Zongyi Wang Apimook Watcharangkool Lianghong Wei Wei Wei Yadong Wei Liangjian Wen Christopher Wiebusch Steven Chan-Fai Wong Bjoern Wonsak Diru Wu Fangliang Wu Qun Wu Wenjie Wu Zhi Wu Michael Wurm Jacques Wurtz Christian Wysotzki Yufei Xi Dongmei Xia Yuguang Xie Zhangquan Xie Zhizhong Xing Benda Xu Donglian Xu Fanrong Xu Jilei Xu Jing Xu Meihang Xu Yin Xu Yu Xu Baojun Yan Xiongbo Yan Yupeng Yan Anbo Yang Changgen Yang Huan Yang Jie Yang Lei Yang Xiaoyu Yang Yifan Yang Haifeng Yao Zafar Yasin Jiaxuan Ye Mei Ye Ugur Yegin Frédéric Yermia Peihuai Yi Xiangwei Yin Zhengyun You Boxiang Yu Chiye Yu Chunxu Yu Hongzhao Yu Miao Yu Xianghui Yu Zeyuan Yu Chengzhuo Yuan Ying Yuan Zhenxiong Yuan Ziyi Yuan Baobiao Yue Noman Zafar Andre Zambanini Pan Zeng Shan Zeng Tingxuan Zeng Yuda Zeng Liang Zhan Feiyang Zhang Guoqing Zhang Haiqiong Zhang Honghao Zhang Jiawen Zhang Jie Zhang Jingbo Zhang Peng Zhang Qingmin Zhang Shiqi Zhang Tao Zhang Xiaomei Zhang Xuantong Zhang Yan Zhang Yinhong Zhang Yiyu Zhang Yongpeng Zhang Yuanyuan Zhang Yumei Zhang Zhenyu Zhang Zhijian Zhang Fengyi Zhao Jie Zhao Rong Zhao Shujun Zhao Tianchi Zhao Dongqin Zheng Hua Zheng Minshan Zheng Yangheng Zheng Weirong Zhong Jing Zhou Li Zhou Nan Zhou Shun Zhou Xiang Zhou Jiang Zhu Kejun Zhu Honglin Zhuang Liang Zong Jiaheng Zou 《Chinese Physics C》 SCIE CAS CSCD 2021年第2期93-110,共18页
The Jiangmen Underground Neutrino Observatory(JUNO)features a 20 kt multi-purpose underground liquid scintillator sphere as its main detector.Some of JUNO's features make it an excellent location for^8B solar neut... The Jiangmen Underground Neutrino Observatory(JUNO)features a 20 kt multi-purpose underground liquid scintillator sphere as its main detector.Some of JUNO's features make it an excellent location for^8B solar neutrino measurements,such as its low-energy threshold,high energy resolution compared with water Cherenkov detectors,and much larger target mass compared with previous liquid scintillator detectors.In this paper,we present a comprehensive assessment of JUNO's potential for detecting^8B solar neutrinos via the neutrino-electron elastic scattering process.A reduced 2 MeV threshold for the recoil electron energy is found to be achievable,assuming that the intrinsic radioactive background^(238)U and^(232)Th in the liquid scintillator can be controlled to 10^(-17)g/g.With ten years of data acquisition,approximately 60,000 signal and 30,000 background events are expected.This large sample will enable an examination of the distortion of the recoil electron spectrum that is dominated by the neutrino flavor transformation in the dense solar matter,which will shed new light on the inconsistency between the measured electron spectra and the predictions of the standard three-flavor neutrino oscillation framework.IfDelta m^(2)_(21)=4.8times10^(-5);(7.5times10^(-5))eV^(2),JUNO can provide evidence of neutrino oscillation in the Earth at approximately the 3sigma(2sigma)level by measuring the non-zero signal rate variation with respect to the solar zenith angle.Moreover,JUNO can simultaneously measureDelta m^2_(21)using^8B solar neutrinos to a precision of 20% or better,depending on the central value,and to sub-percent precision using reactor antineutrinos.A comparison of these two measurements from the same detector will help understand the current mild inconsistency between the value of Delta m^2_(21)reported by solar neutrino experiments and the KamLAND experiment. 展开更多
关键词 neutrino oscillation solar neutrino JUNO
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