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基于InSAR技术的伊宁县滑坡早期识别

中国矿业 2024年第10期33卷 131-142页

作者：张蕙张娅娣师芸西安科技大学安全科学与工程学院陕西西安710054 陕西交通职业技术学院建筑与测绘工程学院陕西西安710018 西安科技大学测绘科学与技术学院陕西西安710054

针对伊犁地区受冻融作用和降水影响致使境内滑坡灾害频发的现状,本文以伊宁县为研究对象,联合2020年1月至2021年12月的Sentinel-A数据和2016年5月至2020年5月的ALOS-2数据,采用Stacking-InSAR技术和SBAS-InSAR技术获取研究区地表形变信... 详细信息

针对伊犁地区受冻融作用和降水影响致使境内滑坡灾害频发的现状,本文以伊宁县为研究对象,联合2020年1月至2021年12月的Sentinel-A数据和2016年5月至2020年5月的ALOS-2数据,采用Stacking-InSAR技术和SBAS-InSAR技术获取研究区地表形变信息,结合光学遥感解译共识别潜在滑坡418处,并对典型地质灾害区域滑坡识别结果进行了野外验证。分析两种时序InSAR技术的优缺点,构建了伊宁县滑坡InSAR早期识别方法。引入降水量数据结合伊宁县气候特征对胡吉尔特滑坡群时空演化特征进行分析,推断可知冻融作用和降雨为区内滑坡灾害的主要诱发因子,且冻融期形变速率大于降雨期。区内滑坡主要分布在坡度10°~30°,坡向以阴坡为主,距断裂带小于5 km的互层状较软弱以砂岩、砾岩、砂砾石和亚砂土为主的岩组。研究结果表明了InSAR技术识别伊宁县滑坡的可靠性,可为当地灾害防治提供技术参考和科学依据。

关键词： InSAR 伊宁县潜在滑坡冻融作用发育特征

Target-oriented Q-compensated reverse-time migration by using optimized pure-mode wave equation in anisotropic media

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Petroleum Science 2023年第2期20卷 866-878页

作者： shi-Gang Xu Qian-Zong Bao zhi-Ming Ren chang'an university School of Geological Engineering and GeomaticsDepartment of GeophysicsXi'anShaanxi710064China National engineering Research Center of Offshore Oil and Gas Exploration Beijing100028China

Research on seismic anisotropy and attenuation plays a significant role in exploration geophysics. To enhance the imaging quality for complicated structures, we develop several effective improvements for anisotropic attenuation effects in reverse-time migration (Q-RTM) on surface and vertical seismic profiling (VSP) acquisition geometries. First, to suppress pseudo-shear wave artifact and numerical instability of the commonly used anisotropic pseudo-acoustic wave equations, an optimized pure P-wave dispersion relation is derived and the corresponding pure-mode wave equation is solved by combining the finite-difference and Possion methods. Second, a simplified anisotropic pure-mode visco-acoustic wave equation (PVAWE) based on standard linear solid model is established. Third, a time-dispersion correlation strategy is applied to improve the modeling accuracy. Fourth, we extend a target-oriented scheme to anisotropic attenuated modeling and imaging. Instead of the conventional wavefield modeling and RTM, the proposed approach can extract available wavefield information near the target regions and produce high imaging resolution for target structures. Last, both anisotropic surface and VSP Q-RTMs are executed by combining optimized PVAWE, time-dispersion correlation and target-oriented algorithm. Modeling examples demonstrate the advantages of our schemes. Moreover, our modified Q-compensated imaging workflow can be regarded as a supplement to the classical anisotropic RTM.

关键词： Anisotropy Attenuation Reverse-time migration Wave equation Optimized algorithm Target-oriented

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最小曲率位场分离方法参数选择试验研究

地球物理学进展 2019年第4期34卷 1441-1452页

作者：纪晓琳王万银邱之云长安大学重磁方法技术研究所长安大学地质工程与测绘学院长安大学西部矿产资源与地质工程教育部重点实验室

位场分离是位场解释中最困难的问题之一.本文作者曾在2015年研究了单步长非原位和原位迭代两种类型最小曲率位场分离差分迭代格式,并利用Fourier频谱分析理论研究了这两种类型迭代格式的收敛性及位场分离效果,在实际应用中如何选择有关... 详细信息

位场分离是位场解释中最困难的问题之一.本文作者曾在2015年研究了单步长非原位和原位迭代两种类型最小曲率位场分离差分迭代格式,并利用Fourier频谱分析理论研究了这两种类型迭代格式的收敛性及位场分离效果,在实际应用中如何选择有关参数就是本文研究的内容.首先,利用理论模型对迭代步长和迭代次数选择进行了模型试验,模型试验显示单步长原位迭代和叠加步长原位迭代均能收敛、且能获得较好的位场分离效果;迭代步长可根据位场分离目的选取,当位场异常迭代最大残差差值和原场均值平均相对误差差值趋于0时的迭代次数为最佳迭代次数;其次,三层组合模型位场分离试验再次验证了原位迭代最小曲率位场分离方法的有效性.最后,利用西非中南段加蓬盆地卫星测高重力异常数据处理试验显示了最小曲率位场分离方法的实用性.

关键词：最小曲率原位迭代单步长叠加步长迭代步长迭代次数位场分离

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聚丙烯纤维加筋黄土的抗剪强度和崩解特性

交通运输工程学报 2021年第2期21卷 82-92页

作者：卢浩晏长根贾卓龙兰恒星石玉玲杨晓华张志权广东华路交通科技有限公司广东广州510420 长安大学公路学院陕西西安710064 长安大学地质工程与测绘学院陕西西安710054 长安大学建筑工程学院陕西西安710064

为检验聚丙烯纤维加筋黄土对边坡坡面的防护效果,基于室内直剪试验和崩解试验,研究了纤维含量、纤维长度及含水率对加筋黄土抗剪强度和抗崩解特性的影响,获得了加筋黄土的最佳配比,并以此为基础开展了现场坡面防护试验。研究结果表明:... 详细信息

为检验聚丙烯纤维加筋黄土对边坡坡面的防护效果,基于室内直剪试验和崩解试验,研究了纤维含量、纤维长度及含水率对加筋黄土抗剪强度和抗崩解特性的影响,获得了加筋黄土的最佳配比,并以此为基础开展了现场坡面防护试验。研究结果表明:相比于素黄土,聚丙烯纤维加筋黄土的黏聚力最高提升113.8%,内摩擦角最高提升23.3%,崩解速率最高降低87.5%,聚丙烯纤维可有效提高黄土的抗剪强度和抗崩解特性;随着纤维含量和纤维长度的增长,聚丙烯纤维加筋黄土的黏聚力分别呈现先增大后减小和先急剧增大后增幅趋缓的变化趋势,崩解速率分别呈现先减小后增加和持续减小的变化趋势;从抗剪强度方面考虑,聚丙烯纤维加筋黄土的最佳纤维含量为0.3%,最佳纤维长度为15 mm,从崩解特性方面考虑,聚丙烯纤维加筋黄土的最佳纤维含量为0.5%,最佳纤维长度为19 mm,相比较而言,两者崩解速率的相对变化明显小于其抗剪强度的相对变化,故确定聚丙烯纤维加筋黄土的最佳纤维含量为0.3%,最佳纤维长度为15 mm;随着含水率的增加,聚丙烯纤维加筋黄土的黏聚力、内摩擦角和崩解速率均呈现减小趋势,其变化关系符合三次多项式函数或Logistic函数关系;现场测得聚丙烯纤维加筋黄土防护坡面平均侵蚀深度约为3 mm,说明聚丙烯纤维加筋黄土的坡面防护效果明显。

关键词：路基工程加筋黄土聚丙烯纤维抗剪强度崩解速率

典型油藏CO2地质封存中四维地震正演模型研究

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地球物理学进展 2018年第6期33卷 2383-2393页

作者：李琳马劲风王浩璠谭明友崔世凌张云银曲志鹏二氧化碳捕集与封存技术国家地方联合工程研究中心西北大学地质学系西安710069 中国石油化工股份有限公司胜利油田分公司物探研究院山东东营257022

在CO_2地质封存中,储层中流体饱和度以及地层压力都会随着CO_2的注入而发生变化,相应的纵横波速度也会发生变化.本文首先进行原始状态下横波速度的预测,利用考虑了压力变化的Hertz-Mindlin公式结合Gassmann方程计算横波速度,为了进行对... 详细信息

在CO_2地质封存中,储层中流体饱和度以及地层压力都会随着CO_2的注入而发生变化,相应的纵横波速度也会发生变化.本文首先进行原始状态下横波速度的预测,利用考虑了压力变化的Hertz-Mindlin公式结合Gassmann方程计算横波速度,为了进行对比,又采用不考虑压力变化的Castagna经验公式来进行横波速度的预测.然后,利用这两种方法进行流体替换之后的纵、横波速度的预测,为了体现压力的影响,分别做了(1)利用Hertz-Mindlin公式以及Gassmann方程计算流体替换之后的纵、横波速度;(2)利用Hertz-Mindlin公式以及Gassmann方程计算流体替换之后的纵、横波速度,不考虑压力的变化,即流体替换前后压力不变;(3)利用Hertz-Mindlin公式以及Gassmann方程计算纵、横波速度,仅考虑压力的变化而假设饱和度不变;(4)利用Gastagna经验公式计算流体替换之后的纵、横波速度.在完成流体替换前后纵、横波速度的预测之后,又制作了两层模型以及井模型的AVO正演模型.结果表明,只有同时考虑饱和度以及压力的变化才是最符合实际的,而在该区压力的变化所引起的地震响应的变化远远大于饱和度变化所引起的地震响应.本文的研究区块位于胜利油田正理庄油田高89区,所用资料为该区的全波列测井高94井.

关键词：压力饱和度纵波速度横波速度正演模型四维地震

氮素在西部煤矿区地下水库迁移转化的实验研究

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氮素在西部煤矿区地下水库迁移转化的实验研究

中国煤炭学会土地复垦与生态修复专业委员会第八届全国矿区土地复垦与生态修复学术会议

作者：赵丽张垒杨志斌张庆孙超 LUO Shao-he WANG shi-dong TIAN yun-fei MENG Jia-xin ZHANG zhi-ji 河南理工大学资源环境学院中原经济区煤层(页岩)气河南省协同创新中心矿山地质灾害成灾机理与防控重点实验室中煤科工集团西安研究院有限公司 Department of Resource & Environmental engineering Henan polytechnic University Collaborative Innovation Center of Coalbed Methane and Shale Gas for Central Plains Economic Region Key Laboratory of Mine geological Hazards Mechanism and Control CCTEG xi'an Research institute

基于浅埋深、薄基岩、厚煤层的赋存条件,在我国西部煤矿区往往排出富含有机氮和无机氮(硝酸盐氮、亚硝酸盐氮或氨氮)的矿井水,如果不经过处理就直接排放,会给生态环境带来严重危害。作为实现保水采煤、生态保护的措施之一,地下水库技术... 详细信息

基于浅埋深、薄基岩、厚煤层的赋存条件,在我国西部煤矿区往往排出富含有机氮和无机氮(硝酸盐氮、亚硝酸盐氮或氨氮)的矿井水,如果不经过处理就直接排放,会给生态环境带来严重危害。作为实现保水采煤、生态保护的措施之一,地下水库技术已在我国多个西部生态脆弱煤矿区得到了实施,然而有关水质保障及安全运行的研究报道甚少。研究通过矸石柱模拟补连塔矿地下水库的水文地质环境,结合水中TN、"三氮"等理化指标的测试,开展了矿井水中氮素的迁移转化规律研究。研究结果表明:渗流流量均值0.51 mL/min、1 016h(12.54个孔隙体积数PV)内,在模拟的水-岩间的缺氧环境中,同时存在有机氮的矿化作用、亚硝酸盐及硝酸盐的反硝化作用。在实验初期的1.19～2.47PV,有机氮浓度快速下降,而氨氮浓度快速上升,这说明试验初期有机氮的氨化作用较强。之后有机氮的矿化作用逐渐减弱,导致水中氨氮含量逐渐减小并趋于稳定。在矿井水C/N为2.32～3.08的条件下,较强的还原作用导致亚硝酸盐的去除率在99.9%以上、硝酸盐的去除效率在74%～90%。矿井水TN的去除效率在57%～71%,由于淋滤用液硝酸盐含量较低,因此TN的去除主要与亚硝酸盐的减少有关。研究结果可为地下水库技术的有效实施提供水质保障和安全运行方面的借鉴。

关键词：西部煤矿区地下水库矿井水氮素煤矸石

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安全工程专业实验教学改革与实践

教育教学论坛 2021年第13期 63-66页

作者：韩冬冬石耀武刘志云李凯玲长安大学地质工程与测绘学院陕西西安710054

工程教育专业认证及新工科建设对安全工程专业实验教学提出了新要求,从实验课程设置、教学内容、教学方法及考核方式等四个方面分析了安全工程实验教学中存在的问题。提出了独立设置实验课与课内实验共存,增加了紧跟科技、经济发展的实... 详细信息

工程教育专业认证及新工科建设对安全工程专业实验教学提出了新要求,从实验课程设置、教学内容、教学方法及考核方式等四个方面分析了安全工程实验教学中存在的问题。提出了独立设置实验课与课内实验共存,增加了紧跟科技、经济发展的实验内容,采取了“以学生为中心”的多样化教学方法和“以产出为导向”的过程考核方式,并提出了持续改进的建议。可为高校安全工程及其他相关专业提供借鉴。

关键词：安全工程实验教学改革与实践

Feasibility and physics potential of detecting ^(8)B solar neutrinos at JUNO

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Chinese Physics C 2021年第2期45卷 93-110页

作者： Angel Abusleme Thomas Adam 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 Yan Yerevan Physics institute YerevanArmenia Universitélibre de Bruxelles BrusselsBelgium Universidade Estadual de Londrina LondrinaBrazil Pontificia Universidade Catolica do Rio de Janeiro RioBrazil Pontificia Universidad Católica de Chile SantiagoChile Universidad Tecnica Federico Santa Maria ValparaisoChile Beijing institute of Spacecraft Environment engineering BeijingChina Beijing Normal university BeijingChina china institute of Atomic Energy BeijingChina institute of High Energy Physics BeijingChina North china Electric Power university BeijingChina School of Physics Peking UniversityBeijingChina Tsinghua university BeijingChina university of Chinese Academy of Sciences BeijingChina Jilin university ChangchunChina College of Electronic Science and engineering National University of Defense TechnologyChangshaChina Chongqing university ChongqingChina Dongguan university of Technology DongguanChina Jinan university GuangzhouChina Sun Yat-Sen university GuangzhouChina Harbin institute of Technology HarbinChina university of Science and Technology of china HefeiChina The Radiochemistry and Nuclear Chemistry Group in university of South china HengyangChina Wuyi university JiangmenChina Shandong university JinanChina institute of Modern Physics Chinese Academy of SciencesLanzhouChina Nanjing university NanjingChina Guangxi university NanningChina East china university of Science and Technology ShanghaiChina School of Physics and Astronomy Shanghai Jiao Tong UniversityShanghaiChina Tsung-Dao Lee institute Shanghai Jiao Tong UniversityShanghaiChina institute of Hydrogeology and Environmental Geology Chinese Academy of Geological SciencesShijiazhuangChina Nankai university TianjinChina Wuhan university WuhanChina xi’an Jiaotong university Xi’anChina xiamen university XiamenChina School of Physics and Microelectronics Zhengzhou UniversityZhengzhouChina institute of Physics National Chiao-Tung university Hsinchu National United university Miao-Li Department of Physics National T

The Jiangmen Underground Neutrino Observatory(JUNO)features a 20 kt multi-purpose underground liquid scintillator sphere as its main *** 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 *** 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/*** ten years of data acquisition,approximately 60,000 signal and 30,000 background events are *** 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 *** 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 ***,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.

关键词： neutrino oscillation solar neutrino JUNO

Sub-percent precision measurement of neutrino oscillation parameters with JUNO

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Chinese Physics C 2022年第12期46卷 28-49页

作者： Angel Abusleme Thomas Adam 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 Ho Yerevan Physics institute YerevanArmenia Universiélibre de Bruxelles BrusselsBelgium Universidade Estadual de Londrina LondrinaBrazil Pontificia Universidade Catolica do Rio de Janeiro Rio de JaneiroBrazil Pontificia Universidad Católica de Chile SantiagoChile Universidad Tecnica Federico Santa Maria ValparaisoChile Beijing institute of Spacecraft Environment engineering BeijingChina Beijing Normal university BeijingChina china institute of Atomic Energy BeijingChina institute of High Energy Physics BeijingChina North china Electric Power university BeijingChina School of Physics Peking UniversityBeijingChina Tsinghua university BeijingChina university of Chinese Academy of Sciences BeijingChina Jilin university ChangchunChina College of Electronic Science and engineering National University of Defense TechnologyChangshaChina Chongqing university ChongqingChina Dongguan university of Technology DongguanChina Jinan university GuangzhouChina Sun Yat-Sen university GuangzhouChina Harbin institute of Technology HarbinChina university of Science and Technology of china HefeiChina The Radiochemistry and Nuclear Chemistry Group in university of South china HengyangChina Wuyi university JiangmenChina Shandong university JinanChinaand Key Laboratory of Particle Physics and Particle Irradiation of Ministry of EducationShandong UniversityQingdaoChina institute of Modern Physics Chinese Academy of SciencesLanzhouChina Nanjing university NanjingChina Guangxi university NanningChina East china university of Science and Technology ShanghaiChina School of Physics and Astronomy Shanghai Jiao Tong UniversityShanghaiChina Tsung-Dao Lee institute Shanghai Jiao Tong UniversityShanghaiChina institute of Hydrogeology and Environmental Geology Chinese Academy of Geological SciencesShijiazhuangChina Nankai university TianjinChina Wuhan university WuhanChina xi'an Jiaotong university Xi'anChina xiamen university XiamenChina School of Physics and Microelectronics Zhengzhou UniversityZhengzhou

JUNO is a multi-purpose neutrino observatory under construction in the south of *** publication presents new sensitivity estimates for the measurement of the △m_(31)^(2),△m_(21)^(2),sin^(2)θ_(12),and sin^(2)θ_(13) oscillation parameters using reactor antineutrinos,which is one of the primary physics goals of 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 *** is found that the △m_(21)^(2) and sin^(2)θ_(12) oscillation parameters will be determined to 0.5%precision or better in six years of data *** the same period,the △m_(31)^(2) parameter will be determined to about 0.2%precision for each mass ordering *** new precision represents approximately an order of magnitude improvement over existing constraints for these three parameters.

关键词： neutrino oscillation reactor antineutrino precision measurement JUNO