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Effects of foliation angle on mechanical characteristics of carbonaceous slate using uniaxial compression tests
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作者 Yuanguang Zhu Xuanyao Wang +2 位作者 Bin liu xuewei liu Haoyuan Xue 《Journal of Rock Mechanics and Geotechnical Engineering》 2025年第4期2091-2108,共18页
Carbonaceous slate is one kind of metamorphic rocks with developed foliation,which is frequently encountered during tunnel construction in Western China.The foliation plays a crucial role in the stability of tunnels.F... Carbonaceous slate is one kind of metamorphic rocks with developed foliation,which is frequently encountered during tunnel construction in Western China.The foliation plays a crucial role in the stability of tunnels.For this,we conducted uniaxial compression tests,acoustic emission(AE)monitoring and scanning electron microscope(SEM)tests on carbonaceous slate.The results show that the strength,failure mode,and AE characteristics exhibit marked anisotropy with the angle between the axial and the foliation(β).Asβincreases,the ultrasonic wave velocity decreases monotonically,whereas the uniaxial compressive strength(UCS)displays a distinctive U-shaped trend.The elastic modulus initially decreases and then increases.The cumulative AE counts curve and energy curve show a stepped growth whenβ≤45°.The AE events are active during the crack compaction phase and remain calm during the linear elastic deformation phase whenβ>45°.Upon failure,the energy release accounts for the highest proportion(67%)whenβ=45°,while the proportions in other cases are less than 37%.The maximum percentage(31%)of shear cracks is reported whenβ=60°,which is six times greater than that atβ=0°.Moreover,Kernel density estimation analysis reveals that the high concentration area with low AF(AE counts/duration time)and high RA(rise time/amplitude)increases initially,and then decreases whenβ>60°.In addition,nine types of cracks and seven modes of failure were identified.The foliation angle has a pronounced impact on shear failure modes in comparison with tensile failure modes.The supports could suffer larger deformation whenβ≥60°compared to other cases.The failure behaviors correspond well with field observations. 展开更多
关键词 Carbonaceous slate Mechanical behavior Fracture mechanism Acoustic emission ANISOTROPY
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The Water Flooding Seepage Mechanism in the Inter-Fractures of Horizontal Wells in Tight Oil Reservoirs
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作者 Xinli Zhao Qianhua Xiao +3 位作者 xuewei liu Yu Shi Xiangji Dou Guoqiang Xing 《Fluid Dynamics & Materials Processing》 2025年第2期427-444,共18页
Tight oil reservoirs face significant challenges,including rapid production decline,low recovery rates,and a lack of effective energy replenishment methods.In this study,a novel development model is proposed,based on ... Tight oil reservoirs face significant challenges,including rapid production decline,low recovery rates,and a lack of effective energy replenishment methods.In this study,a novel development model is proposed,based on inter-fracture injection following volumetric fracturing and relying on a high-temperature and high-pressure large-scale physical simulation system.Additionally,the CMG(Computer Modelling Group Ltd.,Calgary City,Canada)software is also used to elucidate the impact of various single factors on the production of horizontal wells while filtering out the interference of others.The effects of fracture spacing,fracture half-length,and the injection-production ratio are studied.Results indicate that under rejection pressures of 6.89,3.45,and 1.88 MPa,the times to establish stable flow are 50,193,and 395 min,respectively.Higher injection pressures lead to an increased oil recovery efficiency,with the highest observed efficiency at 16.93%.This indicates that,compared with conventional medium and high permeability reservoirs,tight oil reservoirs exhibit similar pore throats and larger capillary forces when oil and water flow in both phases.Higher pressures reduce capillary forces,displacing more oil droplets,thus enhancing oil recovery efficiency.Moreover,under inter-fracture displacement conditions,the pressure gradient at both the injection and production ends remain consistent,with minimal pressure loss near the wellbore.This feature ensures that the crude oil in the middle of the reservoir also possesses displacement energy,thereby enhancing overall crude oil displacement efficiency. 展开更多
关键词 Tight oil reservoir volumetric fracturing inter-fracture injection and production oil drive efficiency WATERFLOODING
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Grouting Flow in Deep Fractured Rock:A State-of-the-Art Review of Theory and Practice
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作者 xuewei liu Jinze Sun +4 位作者 Bin liu Yongshui Kang Yongchao Tian Yuan Zhou Quansheng liu 《Fluid Dynamics & Materials Processing》 2025年第8期2047-2073,共27页
Grouting is a widely applied technique for reinforcing fractured zones in deep soft rock tunnels.By infiltrating rock fissures,slurry materials enhance structural integrity and improve the overall stability of the sur... Grouting is a widely applied technique for reinforcing fractured zones in deep soft rock tunnels.By infiltrating rock fissures,slurry materials enhance structural integrity and improve the overall stability of the surrounding rock.The performance of grouting is primarily governed by the flow behavior and diffusion extent of the slurry.This review considers recent advances in the theory and methodology of slurry flow and diffusion in fractured rock.It examines commonly used grout materials,including cement-based,chemical,and composite formulations,each offering distinct advantages for specific geological conditions.Themechanisms of reinforcement vary significantly across materials,requiring tailored application strategies.The rheological properties of grouting slurries,particularly cement-based types,have been widely modeled using classical constitutive approaches.However,the influence of time-and space-dependent viscosity evolution on slurry behavior remains underexplored.Experimental studies have provided valuable insights into slurry diffusion,yet further research is needed to capture real-time behavior under multi-scale and multi-physics coupling conditions.Similarly,current numerical simulations are largely limited to twoand three-dimensional models of single-fracture flow.These models often neglect the complexity of fracture networks and geological heterogeneity,highlighting a need for more realistic and integrated simulation frameworks.Future research should focus on:(1)fine-scale modeling of slurry hydration and mechanical reinforcement processes;(2)cross-scale analysis of slurry flow under coupled thermal,hydraulic,andmechanical fields;and(3)development of realtime,three-dimensional dynamic simulation tools to capture the full grouting process.These efforts will strengthen the theoretical foundation and practical effectiveness of grouting in complex underground environments. 展开更多
关键词 Grouting material rheological characterization diffusion behavior numerical simulation method
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Seismic Attenuation and Velocity Dispersion to Discriminate Gas Hydrates and Free Gas Zone, Makran Offshore, Pakistan
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作者 Muhammad Irfan Ehsan Perveiz Khalid +3 位作者 Nisar Ahmed Jiachun You xuewei liu Tahir Azeem 《International Journal of Geosciences》 2016年第8期1020-1028,共9页
Gas hydrates gained a remarkable attention as an unconventional energy resource recently. In order to interpret gas hydrates (part of fluid) and free gas saturated zone accurately, it is essential to implement new tec... Gas hydrates gained a remarkable attention as an unconventional energy resource recently. In order to interpret gas hydrates (part of fluid) and free gas saturated zone accurately, it is essential to implement new technique related to seismic attenuation and velocity dispersion. P wave attenuation and velocity dispersion in porous media made promising imprints for exploration of gas hydrates. The most prominent phenomenon for attenuation and velocity dispersion in porous media is wave induced fluid flow in which wave inhomogeneities are larger than pore size but smaller than wavelength. Numerical simulation technique is applied to analyze frequency dependent velocity dispersion and attenuation in gas hydrates and free gas layer in Makran offshore of Pakistan. Homogeneous and patchy distribution patterns of gas hydrates and free gas within pore spaces of host sediments at lower and higher frequency regime are considered. It is noted that the attenuation and velocity dispersion increase with the increase in gas hydrates saturation. The maximum attenuation is observed at 66% saturation of gas hydrates in the area under investigation. However, in case of water and gas mixture the maximum attenuation and velocity dispersion occur at low gas saturation (~15%). Therefore, based on our numerical simulation, velocity dispersion and attenuation can be used as seismic attributes to differentiate various gas saturations and gas hydrates saturation for Makran offshore area of Pakistan. 展开更多
关键词 Gas Hydrates Seismic Attenuation Velocity Dispersion Makran Offshore Seismic Attributes
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石墨烯包覆天然球形石墨作为锂离子电池的负极材料,是否需要乙炔黑导电剂? 被引量:7
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作者 刘学伟 牛莹 +3 位作者 曹瑞雄 陈晓红 商红岩 宋怀河 《物理化学学报》 SCIE CAS CSCD 北大核心 2022年第2期95-103,共9页
我们通过包覆炭化的方法制备得到了石墨烯包覆的天然球形石墨(G/SG)材料,并使用扫描电子显微镜、X射线衍射仪以及多种电化学测试手段考察了不同石墨烯含量的复合材料的形貌结构及电化学性能。我们发现,在不添加乙炔黑(AB)的情况下,G/SG... 我们通过包覆炭化的方法制备得到了石墨烯包覆的天然球形石墨(G/SG)材料,并使用扫描电子显微镜、X射线衍射仪以及多种电化学测试手段考察了不同石墨烯含量的复合材料的形貌结构及电化学性能。我们发现,在不添加乙炔黑(AB)的情况下,G/SG复合材料表现出较高的首次库伦效率,很好的循环稳定性和高倍率性能。当石墨烯包覆量为1%时,材料50次循环后的可逆容量可与添加10%AB的天然石墨电极(SG)等同;当石墨烯包覆量为2.5%时,材料的比容量完全高于添加10%AB的石墨电极。材料电化学性能的改善归因于石墨烯的包覆。一方面,石墨烯的柔软可变性可以保证天然石墨颗粒在充放电过程中的结构完整性,从而有效改善材料的循环稳定性;另一方面,石墨烯的存在提高了电极的导电性,促进更好导电网络的形成。因此,石墨烯包覆天然球形石墨材料中,石墨烯不仅是活性物质,也发挥导电剂的作用。当添加5%的乙炔黑时,在50 mA·g^(-1)电流循环50次后,5%G/SG电极的可逆容量从381.1 mAh·g^(-1)提高到404.5 mAh·g^(-1),在1 A·g^(-1)电流时可逆容量从82.5 mAh·g^(-1)提高到101.9 mAh·g^(-1),这表明G/SG电极仍然需要乙炔黑导电剂。乙炔黑颗粒填充在复合材料的空隙中,通过点接触的形式连接到G/SG颗粒,与石墨烯协同作用形成了更加有效的导电网络。尽管石墨烯包覆和乙炔黑添加对天然石墨电极具有积极的影响,例如增加了天然石墨电极的导电性和储锂性能(包括可逆容量,倍率性能和循环性能),但随着石墨烯或乙炔黑的增加,电极密度通常会降低。因此,在实际应用中应考虑石墨负极材料的质量和体积容量的平衡。这些结果对天然石墨的进一步商业应用具有重要意义。我们的工作为天然石墨电极在锂电池中的电化学行为提供了一种新的认识,并且有助于制备更高性能的负极材料。 展开更多
关键词 石墨烯 石墨烯包覆 天然球形石墨 锂离子电池 负极材料 导电剂 乙炔黑
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A real-time prediction method for tunnel boring machine cutter-head torque using bidirectional long short-term memory networks optimized by multi-algorithm 被引量:7
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作者 Xing Huang Quantai Zhang +4 位作者 Quansheng liu xuewei liu Bin liu Junjie Wang Xin Yin 《Journal of Rock Mechanics and Geotechnical Engineering》 SCIE CSCD 2022年第3期798-812,共15页
Based on data from the Jilin Water Diversion Tunnels from the Songhua River(China),an improved and real-time prediction method optimized by multi-algorithm for tunnel boring machine(TBM)cutter-head torque is presented... Based on data from the Jilin Water Diversion Tunnels from the Songhua River(China),an improved and real-time prediction method optimized by multi-algorithm for tunnel boring machine(TBM)cutter-head torque is presented.Firstly,a function excluding invalid and abnormal data is established to distinguish TBM operating state,and a feature selection method based on the SelectKBest algorithm is proposed.Accordingly,ten features that are most closely related to the cutter-head torque are selected as input variables,which,in descending order of influence,include the sum of motor torque,cutter-head power,sum of motor power,sum of motor current,advance rate,cutter-head pressure,total thrust force,penetration rate,cutter-head rotational velocity,and field penetration index.Secondly,a real-time cutterhead torque prediction model’s structure is developed,based on the bidirectional long short-term memory(BLSTM)network integrating the dropout algorithm to prevent overfitting.Then,an algorithm to optimize hyperparameters of model based on Bayesian and cross-validation is proposed.Early stopping and checkpoint algorithms are integrated to optimize the training process.Finally,a BLSTMbased real-time cutter-head torque prediction model is developed,which fully utilizes the previous time-series tunneling information.The mean absolute percentage error(MAPE)of the model in the verification section is 7.3%,implying that the presented model is suitable for real-time cutter-head torque prediction.Furthermore,an incremental learning method based on the above base model is introduced to improve the adaptability of the model during the TBM tunneling.Comparison of the prediction performance between the base and incremental learning models in the same tunneling section shows that:(1)the MAPE of the predicted results of the BLSTM-based real-time cutter-head torque prediction model remains below 10%,and both the coefficient of determination(R^(2))and correlation coefficient(r)between measured and predicted values exceed 0.95;and(2)the incremental learning method is suitable for realtime cutter-head torque prediction and can effectively improve the prediction accuracy and generalization capacity of the model during the excavation process. 展开更多
关键词 Tunnel boring machine(TBM) Real-time cutter-head torque prediction Bidirectional long short-term memory (BLSTM) Bayesian optimization Multi-algorithm fusion optimization Incremental learning
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Experimental and numerical investigation on failure characteristics and mechanism of coal with different water contents 被引量:4
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作者 xuewei liu Haixiao Chen +4 位作者 Bin liu Sai Wang Quansheng liu Yong Luo Jin Luo 《International Journal of Coal Science & Technology》 EI CAS CSCD 2023年第4期325-342,共18页
Water injection, as a widely used technique to prevent coal burst, can restrain the fractured coal seam and released the energy storage. In this study, laboratory tests were frstly carried out on standard coal specime... Water injection, as a widely used technique to prevent coal burst, can restrain the fractured coal seam and released the energy storage. In this study, laboratory tests were frstly carried out on standard coal specimens with fve diferent water contents (i.e., 0%, 0.6%, 1.08%, 1.5%, 2.0%, and 2.3%). The failure mode, fragment size, and energy distribution characteristics of coal specimens were investigated. Experimental results show that strength, elastic strain energy, dissipated energy, brittleness index, as well as impact energy index decrease with increasing water content. Besides, the failure mode transitions gradually from splitting ejection to tensile-shear mixed failure mode as water content increases, and average fragment size shows positively related to water content. Moreover, scanning electron microscope tests results indicate that water in coal sample mainly causes the mineral softening and defects increase. Furthermore, a numerical model containing roadway excavation was established considering the water on coal burst prevention. Modelling results revealed that water injection can reduce degree of coal burst and ejection velocity of coal blocks, while it will raise up the depth of crack zone and surface displacement of roadway. Combined with laboratory tests and numerical results, the micro mechanism, energy mechanism, and engineering signifcance of water injection on coal burst prevention were fnally analyzed. 展开更多
关键词 Water content Coal burst Failure mode ENERGY Numerical simulation
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On the Development of an Effective Pressure Driving System for Ultra-Low Permeability Reservoirs 被引量:4
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作者 Yapu Zhang Zhengming Yang +2 位作者 Dajian Li xuewei liu Xinli Zhao 《Fluid Dynamics & Materials Processing》 EI 2021年第6期1067-1075,共9页
Given its relevance to the exploitation of ultra-low permeability reservoirs,which account for a substantial proportion of the world’s exploited and still unexploited reserves,in the present study the development of ... Given its relevance to the exploitation of ultra-low permeability reservoirs,which account for a substantial proportion of the world’s exploited and still unexploited reserves,in the present study the development of an adequate water injection system is considered.Due to the poor properties and weak seepage capacity of these reservoirs,the water injection pressure typically increases continuously during water flooding.In this research,the impact on such a process of factors as permeability,row spacing,and pressure gradient is evaluated experimentally using a high-pressure large-scale outcrop model.On this basis,a comprehensive evaluation coefficient is introduced able to account for the effective driving pressure. 展开更多
关键词 Ultra-low permeability reservoir physical simulation effective development water flooding effective driving coefficient
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Experimental and theoretical insights into copper phthalocyanine-based covalent organic frameworks for highly efficien radioactive iodine capture 被引量:3
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作者 xuewei liu Anrui Zhang +7 位作者 Ran Ma Bo Wu Tao Wen Yuejie Ai Mingtai Sun Jie Jin Suhua Wang Xiangke Wang 《Chinese Chemical Letters》 SCIE CAS CSCD 2022年第7期3549-3555,共7页
Exploring efficient materials for capturing radioactive iodine in nuclear waste is of great significance for the progress of nuclear energy as well as the protection of ecological environment.Covalent organic framewor... Exploring efficient materials for capturing radioactive iodine in nuclear waste is of great significance for the progress of nuclear energy as well as the protection of ecological environment.Covalent organic frameworks(COFs)have emerged as promising adsorbents because of their predesignable and functionalizable skeleton structures.However,it remains a grand challenge to achieve large scale preparation of COFs.In this work,we developed a mild and efficient microwave irradiation method instead of the traditional solvothermal method to prepare copper phthalocyanine-based covalent organic frameworks(Cu_(x)Pc-COFs)within only 15 min.The nitrogen-rich 1,2,4,5-tetracarbonitrilebenzene(TCNB)was selected as the solely organic ligand to construct copper phthalocyanine-based 2D conjugated COFs.The resultant Cu_(x)Pc-COFs exhibited excellent iodine enrichment with 2.99 g/g for volatile iodine and 492.27 mg/g for iodine-cyclohexane solution,respectively,outperforming that of many porous materials.As indicated by spectroscopic analysis and DFT calculations,this impressive adsorption performance can be attributed to the charge transfer arising from nitrogen-rich phthalocyanine structures and electron-richπ-conjugated systems with iodine molecules.Moreover,the strong electrostatic interaction between Cu(Ⅱ)on chelate centers and polyiodide anions(I_(x)^(-))also play an important role in the firmly trapping radioactive iodine.Therefore,this study provides a facile and intelligent approach to implement metal-based COFs for the remediation of toxic radioactive iodine. 展开更多
关键词 Cu_(x)Pc-COFs Microwave Iodine adsorption Charge transfer Electrostatic interaction
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Effects of seepage pressure on the mechanical behaviors and microstructure of sandstone 被引量:2
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作者 xuewei liu Juxiang Chen +3 位作者 Bin liu Sai Wang Quansheng liu Jin Luo 《Journal of Rock Mechanics and Geotechnical Engineering》 SCIE CSCD 2024年第6期2033-2051,共19页
Surrounding rocks of underground engineering are subjected to long-term seepage pressure,which can deteriorate the mechanical properties and cause serious disasters.In order to understand the impact of seepage pressur... Surrounding rocks of underground engineering are subjected to long-term seepage pressure,which can deteriorate the mechanical properties and cause serious disasters.In order to understand the impact of seepage pressure on the mechanical property of sandstone,uniaxial compression tests,P-wave velocity measurements,and nuclear magnetic resonance(NMR)tests were conducted on saturated sandstone samples with varied seepage pressures(i.e.0 MPa,3 MPa,4 MPa,5 MPa,6 MPa,7 MPa).The results demonstrate that the mechanical parameters(uniaxial compressive strength,peak strain,elastic modulus,and brittleness index),total energy,elastic strain energy,as well as elastic strain energy ratio,decrease with increasing seepage pressure,while the dissipation energy and dissipation energy ratio increase.Moreover,as seepage pressure increases,the micro-pores gradually transform into meso-pores and macro-pores.This increases the cumulative porosity of sandstone and decreases P-wave velocity.The numerical results indicate that as seepage pressure rises,the number of tensile cracks increases progressively,the angle range of microcracks is basically from 50-120to 80-100,and as a result,the failure mode transforms to the tensile-shear mixed failure mode.Finally,the effects of seepage pressure on mechanical properties were discussed.The results show that decrease in the effective stress and cohesion under the action of seepage pressure could lead to deterioration of strength behaviors of sandstone. 展开更多
关键词 Rock mechanics Mechanical property Seepage pressure Numerical simulation MICROCRACKS
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Gentianine protects hippocampal neurons in a rat model of recurrent febrile convulsion 被引量:1
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作者 xuewei liu Shumin liu +2 位作者 Na Wang Fang Lu Min Cao 《Neural Regeneration Research》 SCIE CAS CSCD 2011年第15期1130-1135,共6页
Gentianine has been shown to have a protective effect on hippocampal CA1 neurons in rats subjected to recurrent febrile convulsion(FC).The present study sought to explore the possible mechanism of gentianine by intr... Gentianine has been shown to have a protective effect on hippocampal CA1 neurons in rats subjected to recurrent febrile convulsion(FC).The present study sought to explore the possible mechanism of gentianine by intraperitoneally injecting gentianine into rats with warm water-induced FC.The results revealed that neuronal organelle injury was slightly ameliorated in the hippocampal CA1 region.The level of glutamate was decreased,but the level of γ-aminobutyric acid was increased,as detected by ninhydrin staining.In addition,glutamate acid decarboxylase expression in hippocampal CA1 was increased,as determined by immunohistochemistry.The results demonstrated that gentianine can ameliorate FC-induced neuronal injury by enhancing glutamate acid decarboxylase activity,decreasing glutamate levels and increasing γ-aminobutyric acid levels. 展开更多
关键词 febrile convulsion gentianine hippocampal neurons neuroprotective effect GLUTAMATE γ-aminobutyric acid neural regeneration
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High-Temperature and Low-Frequency Acoustic Energy Absorption by a Novel Porous Metamaterial Structure 被引量:1
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作者 Qihang liu xuewei liu +1 位作者 Chuanzeng Zhang Fengxian Xin 《Acta Mechanica Solida Sinica》 SCIE EI CSCD 2021年第6期872-883,共12页
In this paper,we propose a novel porous metamaterial structure with an improved acoustic energy absorption performance at high-temperature and in the low-frequency range.In the proposed novel porous metamaterial struc... In this paper,we propose a novel porous metamaterial structure with an improved acoustic energy absorption performance at high-temperature and in the low-frequency range.In the proposed novel porous metamaterial structure,a porous material matrix containing periodically perforated cylindrical holes arranged in a triangular lattice pattern is applied,and additional interlayers of another porous material are introduced around these perforations.The theoretical model is established by adopting the double porosity theory for the interlayer and the cylindrical hole which form an equivalent inclusion and then applying the homogenization method to the porous metamaterial structure formed by the equivalent inclusion and the porous matrix.The temperature-dependent air and material parameters are considered in the extended theoretical model,which is validated by the finite element results obtained by COMSOL Multiphysics.The acoustic or sound energy absorption performance can be improved remarkably at very low frequencies and high temperature.Furthermore,the underlying acoustic energy absorption mechanism inside the unit-cell is investigated by analyzing the distribution of the time-averaged acoustic power dissipation density and the energy dissipation ratio of each constituent porous material.The results reveal that regardless of the temperature,the acoustic energy is mostly dissipated in the porous material with a lower airflow resistivity,while the acoustic energy dissipated in the porous material with a higher airflow resistivity also becomes considerable in the high-frequency range.The novel porous metamaterial structure proposed in this paper can be efficiently utilized to improve the acoustic energy absorption performance at high temperature. 展开更多
关键词 Novel porous metamaterial structure Double porosity theory Homogenization method Acoustic or sound energy absorption High temperature
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Numerical Simulation of Slurry Diffusion in Fractured Rocks Considering a Time-Varying Viscosity 被引量:1
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作者 Lei Zhu Bin liu +3 位作者 xuewei liu Wei Deng Wenjie Yao Ying Fan 《Fluid Dynamics & Materials Processing》 EI 2024年第2期401-427,共27页
To analyze the effects of a time-varying viscosity on the penetration length of grouting,in this study cement slur-ries with varying water-cement ratios have been investigated using the Bingham’sfluidflow equation and ... To analyze the effects of a time-varying viscosity on the penetration length of grouting,in this study cement slur-ries with varying water-cement ratios have been investigated using the Bingham’sfluidflow equation and a dis-crete element method.Afluid-solid coupling numerical model has been introduced accordingly,and its accuracy has been validated through comparison of theoretical and numerical solutions.For different fracture forms(a single fracture,a branch fracture,and a fracture network),the influence of the time-varying viscosity on the slurry length range has been investigated,considering the change in the fracture aperture.The results show that under different fracture forms and the same grouting process conditions,the influence of the time-varying viscosity on the seepage length is 0.350 m. 展开更多
关键词 Time-varying viscosity binghamfluids UDEC numerical simulation grout penetration length aperture
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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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Computational cytometer based on magnetically modulated coherent imaging and deep learning 被引量:1
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作者 Yibo Zhang Mengxing Ouyang +17 位作者 Aniruddha Ray Tairan liu Janay Kong Bijie Bai Donghyuk Kim Alexander Guziak Yi Luo Alborz Feizi Katherine Tsai Zhuoran Duan xuewei liu Danny Kim Chloe Cheung Sener Yalcin Hatice Ceylan Koydemir Omai B.Garner Dino Di Carlo Aydogan Ozcan 《Light: Science & Applications》 SCIE EI CAS CSCD 2019年第1期385-399,共15页
Detecting rare cells within blood has numerous applications in disease diagnostics.Existing rare cell detection techniques are typically hindered by their high cost and low throughput.Here,we present a computational c... Detecting rare cells within blood has numerous applications in disease diagnostics.Existing rare cell detection techniques are typically hindered by their high cost and low throughput.Here,we present a computational cytometer based on magnetically modulated lensless speckle imaging,which introduces oscillatory motion to the magneticbead-conjugated rare cells of interest through a periodic magnetic force and uses lensless time-resolved holographic speckle imaging to rapidly detect the target cells in three dimensions(3D).In addition to using cell-specific antibodies to magnetically label target cells,detection specificity is further enhanced through a deep-learning-based classifier that is based on a densely connected pseudo-3D convolutional neural network(P3D CNN),which automatically detects rare cells of interest based on their spatio-temporal features under a controlled magnetic force.To demonstrate the performance of this technique,we built a high-throughput,compact and cost-effective prototype for detecting MCF7 cancer cells spiked in whole blood samples.Through serial dilution experiments,we quantified the limit of detection(LoD)as 10 cells per millilitre of whole blood,which could be further improved through multiplexing parallel imaging channels within the same instrument.This compact,cost-effective and high-throughput computational cytometer can potentially be used for rare cell detection and quantification in bodily fluids for a variety of biomedical applications. 展开更多
关键词 RARE magnetic SPECKLE
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Orderly Porous Covalent Organic Frameworks-based Materials:Superior Adsorbents for Pollutants Removal from Aqueous Solutions 被引量:24
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作者 Xiaolu liu Hongwei Pang +7 位作者 xuewei liu Qian Li Ning Zhang Liang Mao Muqing Qiu Baowei Hu Hui Yang Xiangke Wang 《The Innovation》 2021年第1期106-134,共29页
Covalent organic frameworks(COFs)are a new type of crystalline porous polymers known for chemical stability,excellent structural regularity,robust framework,and inherent porosity,making them promising materials for ca... Covalent organic frameworks(COFs)are a new type of crystalline porous polymers known for chemical stability,excellent structural regularity,robust framework,and inherent porosity,making them promising materials for capturing various types of pollutants from aqueous solutions.This review thoroughly presents the recent progress and advances of COFs and COF-based materials as superior adsorbents for the efficient removal of toxic heavy metal ions,radionuclides,and organic pollutants.Information about the interaction mechanisms between various pollutants and COF-based materials are summarized from the macroscopic and microscopic standpoints,including batch experiments,theoretical calculations,and advanced spectroscopy analysis.The adsorption properties of various COF-based materials are assessed and compared with other widely used adsorbents.Several commonly used strategies to enhance COF-based materials’adsorption performance and the relationship between structural property and sorption ability are also discussed.Finally,a summary and perspective on the opportunities and challenges of COFs and COF-based materials are proposed to provide some inspiring information on designing and fabricating COFs and COF-based materials for environmental pollution management. 展开更多
关键词 covalent organic frameworks(COFs) heavy metal ions radionuclides organic pollutants interaction mechanism
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Initial performance results of the JUNO detector
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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 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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》 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 m^(2) 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 ^(214)Po alpha decays from natural radioactive sources.The energy non-linearity is calibrated to better than 1%.Intrinsic contaminations of ^(238)U and ^(232)Th 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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