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Radiation Detection technology and Methods 2024年第1期8卷 I0003-I0016,1-1091页

作者： Waleed Abdallah Tiago Carlos Adorno de Freitas Konstantin Afanaciev Shakeel Ahmad Ijaz Ahmed Xiaocong Ai Abid Aleem Wolfgang Altmannshofer Fabio Alves Weiming An Rui An Daniele Paolo Anderle Stefan Antusch Yasuo Arai Andrej Arbuzov Abdesslam Arhrib Mustafa Ashry Sha Bai Yu Bai Yang Bai Vipul Bairathi Csaba Balazs Philip Bambade Yong Ban Tripamo Bandyopadhyay Shou-Shan bao Desmond P.Barber Ayse Bat Varvara Batozskaya Subash Chandra Behera Alexander Belyaev Michele Bertucci Xiao-Jun Bi Yuanjie Bi Tianjian Bian Fabrizio Bianchi Thomas Biekotter Michela Biglietti Shalva Bilanishvili Deng Binglin Denis Bodrov Anton Bogomyagkov Serge Bondarenko Stewart Boogert Maarten Boonekamp Marcello Borri Angelo Bosotti Vincent Boudry Mohammed Boukidi Igor Boyko Ivanka Bozovic Giuseppe Bozzi Jean-Claude Brient Anastasiia Budzinskaya Masroor Bukhari Vladimir Bytev Giacomo Cacciapaglia Hua Cai Wenyong Cai Wujun Cai Yijian Cai Yizhou Cai Yuchen Cai Haiying Cai Huacheng Cai Lorenzo Calibbi Junsong Cang Guofu Cao Jianshe Cao Antoine Chance Xuejun Chang Yue Chang Zhe Chang Xinyuan Chang Wei Chao Auttakit Chatrabhuti Yimin Che Yuzhi Che Bin Chen Danping Chen Fuqing Chen Fusan Chen Gang Chen Guoming Chen Hua-Xing Chen Huirun Chen Jinhui Chen Ji-Yuan Chen Kai Chen Mali Chen Mingjun Chen Mingshui Chen Ning Chen Shanhong Chen Shanzhen Chen Shao-Long Chen Shaomin Chen Shiqiang Chen Tianlu Chen Wei Chen Xiang Chen Xiaoyu Chen Xin Chen Xun Chen Xurong Chen Ye Chen Ying Chen Yukai Chen Zelin Chen Zilin Chen Gang Chen Boping Chen Chunhui Chen Hok Chuen Cheng Huajie Cheng Shan Cheng Tongguang Cheng Yunlong Chi Pietro Chimenti Wen Han Chiu Guk Cho Ming-Chung Chu Xiaotong Chu Ziliang Chu Guglielmo Coloretti Andreas Crivellin Hanhua Cui Xiaohao Cui Zhaoyuan Cui Brunella D'Anzi Ling-Yun Dai Xinchen Dai Xuwen Dai Antonio De Maria Nicola De Filippis Christophe De La Taille Francesca De Mori Chiara De Sio Elisa Del Core Shuangxue Deng Wei-Tian Deng Zhi Deng Ziyan Deng Bhupal Dev Tang Dewen Biagio Di Micco Ran Ding Siqin Dingl Yadong Ding Haiyi Dong Jianin AGH university of Science and {1. Faculty of Physics and Applied Computer ScienceKrakow Anhui university HefeiAnhui Applied Physics Department Federal Urdu University of ArtsScience and TechnologyIslamabad Banaras Hindu university Institute of ScienceVaranasi Bandirma Onyedi Eylul university Bandirma Beihang university Beijing beijing Computational Science Research Center Beijing beijing Conveyi LTD Beijing beijing Glass Research Institute Co. LtdBeijing beijing Institute of {1. Beijing beijing {1. university Beijing Brown university ProvidenceRI Budker Institute of Nuclear Physics Novosibirsk Cadi Ayyad university Laboratory of Fundamental and Applied PhysicsPolydisciplinary FacultyMarrakech Cairo university Giza Center for Theory and Computation National Tsing Hua UniversityHsinchu Central china {1. university WuhanHubei Central South university ChangshaHunan Centro de Fisica Teorica de Particulas Universidade Tecnica de LisboaLisboa Chengdu KaitengSifang Digital Radio&TV Equipment Co. LtdChengduSichuan china academy of engineering physics MianyangSichuan china building {1.s academy Beijing china Center of Advanced Science and {1. Beijing china Institute of Atomic Energy Beijing china Jiliang {1. HangzhouZhejiang china Nuclear Instrument CO. LTDBeijing china {1. of Geosciences Beijing china {1. of Geosciences WuhanHubei china {1. of Mining and technology XuzhouJiangsu china West {1. university NanchongSichuan Chongqing university Department of PhysicsChongqing Chulalongkorn university Bangkok City university of Hong Kong Department of PhysicsHong Kong Cockcroft Institute Daresbury Cornell university IthacaNY CPPM(AMU/IPhU&CNRS/INP) Marseille Dalian Minzu university DalianLiaoning Dalian university of {1. Department of PhysicsDalian Deutsches Elektronen-Synchrotron DESY Hamburg Dzhelepov laboratory of Nuclear Problems of Joint Institute for Nuclear Research(DLNP JINR) Dubna East china {1. Of Science And Technol

The Circular Electron Positron Collider(CEPC)is a large scientific project initiated and hosted by china,fostered through extensive collaboration with international *** complex comprises four accelerators:a 30 GeV Linac,a 1.1.GeV Damping Ring,a Booster capable of achieving energies up to 1.0 GeV,and a Collider operating at varying energy modes(Z,W,H,and tt).The Linac and Damping Ring are situated on the surface,while the subterranean Booster and Collider are housed in a 1.0 km circumference underground tunnel,strategically accommodating future expansion with provisions for a potential Super Proton Proton Collider(SPPC).The CEPC primarily serves as a Higgs *** its baseline design with synchrotron radiation(SR)power of 30 MW per {1.,it can achieve a luminosity of 5×1.^(34)cm^(-2)s^(-1.per interaction point(IP),resulting in an integrated luminosity of 1. ab^(-1.for two IPs over a decade,producing 2.6 million Higgs *** the SR power to 50 MW per {1. expands the CEPC's capability to generate 4.3 million Higgs bosons,facilitating precise measurements of Higgs coupling at sub-percent levels,exceeding the precision expected from the HL-LHC by an order of *** Technical Design Report(TDR)follows the Preliminary Conceptual Design Report(Pre-CDR,201.)and the Conceptual Design Report(CDR,201.),comprehensively detailing the machine's layout,performance metrics,physical design and analysis,technical systems design,R&D and prototyping efforts,and associated civil engineering ***,it includes a cost estimate and a preliminary construction timeline,establishing a framework for forthcoming engineering design phase and site selection *** is anticipated to begin around 2027-2028,pending government approval,with an estimated duration of 8 *** commencement of experiments and data collection could potentially be initiated in the mid-2030s.

关键词： initiated exceeding precise

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NC–UHPC组合梁抗冲击性能的数值研究

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工程科学学报 2024年第2期46卷 354-364页

作者：伍敏黄于倩潘仁胜金浏杜修力长沙理工大学桥梁工程安全控制教育部重点实验室长沙410114 北京工业大学城市减灾与防灾防护教育部重点实验室北京100124

超高性能混凝土(UHPC)材料已成为极具前景的高性能材料,并在冲击和爆炸等防护工程领域中取得了良好的效果.对于普通钢筋混凝土(NC)梁在受到冲击荷载时较易发生局部冲剪破坏,而纯UHPC梁虽可改善其冲击性能,但高昂的造价限制了其进一步的... 详细信息

超高性能混凝土(UHPC)材料已成为极具前景的高性能材料,并在冲击和爆炸等防护工程领域中取得了良好的效果.对于普通钢筋混凝土(NC)梁在受到冲击荷载时较易发生局部冲剪破坏,而纯UHPC梁虽可改善其冲击性能,但高昂的造价限制了其进一步的应用.为了实现结构抗冲击性能和经济的平衡,提出UHPC局部替换和包裹的方案改善钢筋混凝土梁的抗冲击性能.本文设计了NC梁、UHPC梁和NC–UHPC组合梁等不同的研究工况,然后对比分析各个试件的抗冲击性能.结果表明:相比普通钢筋混凝土梁,UHPC局部替换方案可以有效的避免梁的局部冲剪破坏,而UHPC包裹在冲击荷载下梁的破坏模式由冲剪破坏转变为弯曲破坏,两种方案均可有效的减少梁跨中的峰值位移和残余位移;UHPC局部替换相较于包裹方案,梁的跨中峰值位移和残余位移较小,且具有更高的跨中承载能力,在实际过程中建议UHPC局部替换长度取大于2倍梁高以避免局部冲剪破坏.

关键词：超高性能混凝土普通钢筋混凝土组合梁冲击荷载冲剪破坏弯曲破坏

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Trace doping realizing superior electrochemical performance in P2-type Na_(0.50)Li_(0.08)Mn_(0.60)Co_(0.1.)Ni_(0.1.)0_(2)cathode for sodium-ion batteries

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Chinese Chemical Letters 2023年第12期34卷 387-391页

作者： Hongying Hou Jinxu Qiu bao Li Liang Wang Zhuangzhuang Zhang Mengmin Jia Xiaobing Lai Mingming Han Pengyao Yan Dai-Huo {1. Dongmei Dai bao Wang Faculty of material Science and Engineering Kunming University of Science and TechnologyKunming 650093 China Collaborative Innovation Center of Henan Province for Green Manufacturing of Fine Chemicals Key Laboratory of Green Chemical Media and ReactionsMinistry of EducationSchool of Chemistry and Chemical EngineeringHenan Normal UniversityXinxiang 453007China State key {1. of Biochemical Engineering Institute of Process EngineeringChinese Academy of SciencesBeijing 100190China

P2-type layered oxides are receiving significant interest due to their superior structure and intrinsic *** are strenuous attempts to balance the structure stability,phase transition as well as desirable electrochemical performances by inducing anion/cation ions,changing morphology,adjusting valence,*** this work,several same-period elements of Sc,Ti,V,Cr,Fe,Cu and Zn are doped into Na_(0.50)Li_(0.08)Mn_(0.60)Co_(0.1.)Ni_(0.1.)O_(2)cathodes,which are manipulated by ions radii and valence state,further studied by operando X-ray powder diffraction patterns(XRD).As a result,the Cu^(2+)doped cathode performed higher rate capacities(as high as 86 mAh/g even at 1. C)and more stable structures(capacity retention of~89.4%for 1.0 cycles),which owing to the synergistic effect among the tightened TMO_(2)layer,enlarged d-spacing,reduce O-O electrostatic repulsion,ameliorate lattice distortion as well as mitigate ordering of Na^(+)/vacancy.

关键词： P2-type layeredoxide Same-period elements doping Rietveld refinement Operando XRD Sodium-ion battery

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Relationship between fracturing nominal stress and porosity for metal foams under biaxial tension

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Science china(Technological Sciences) 2003年第5期46卷 546-550页

作者： liu Peisheng (刘培生) The key {1. of beam technology and material modification of ministry of education & Department of materials Science and Engineering Beijing Normal University Beijing 100875 China

The relationship between two fracturing nominal stresses and porosity has been put forward for metal foams under biaxial tensile loading, and its mathematical formula is proved to be quite practical with the relative ... 详细信息

关键词： metal foams, foamed metals, porous metals, porous materials.

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基于7Li(p,γ)8Be共振核反应伽马源的光核嬗变实验原理验证研究

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原子能科学技术 2024年第4期58卷 714-720页

作者：叶杉刘伏龙薄楠王浩然程浩李弘伟吴笛杨婉莎魏继红马田丽樊启文王志强刘毅娜宋明哲刘蕴韬贺创业郭冰中国原子能科学研究院北京102413 北京师范大学核科学与技术学院北京100875 北京师范大学射线束技术教育部重点实验室北京100875

光核嬗变可作为长寿命核废料嬗变的一种补充手段.随着强流质子加速器技术的发展,共振核反应γ源的流强可达到较高强度.7Li(p,γ)8Be共振核反应产生的1.8MeV与1.6MeV伽马射线恰好位于巨共振区内,是研究光核嬗变的较好选择.本工作基于中... 详细信息

光核嬗变可作为长寿命核废料嬗变的一种补充手段.随着强流质子加速器技术的发展,共振核反应γ源的流强可达到较高强度.7Li(p,γ)8Be共振核反应产生的1.8MeV与1.6MeV伽马射线恰好位于巨共振区内,是研究光核嬗变的较好选择.本工作基于中国原子能科学研究院2×1.MV串列加速器,利用7Li(p,γ)8Be共振核反应产生的高能伽马射线对1.7Au进行了光核嬗变实验研究.在质子流强081.A的条件下,当金靶厚度为2mm时,反推得到4π方向上的总嬗变率为(58683±2298)s-1.该实验结果为将来利用共振核反应伽马源进行光核嬗变实验研究奠定了技术基础.

关键词：光核嬗变高能伽马射线共振核反应核废料

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Gold nanoparticles attached NH^(2+) ion implantation-modified indium tin oxide electrode:Characterization and electrochemical studies

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Science china Chemistry 2012年第9期55卷 1940-1945页

作者： LI ShuoQi liu Lu HU JingBo key {1. of beam technology and material modification ministry of education Beijing Normal UniversityBeijing 100875China College of Chemistry beijing normal university Beijing 100875China College of Chemistry and Molecular Engineering Peking UniversityBeijing 100870China

An NH2+ ion implantation-modified indium tin oxide film was prepared and the implantation of amino groups on the indium tin oxide substrate was verified by X-ray photoelectron spectroscopy *** gold nanoparticles attached surface could be obtained by self-assembly of different sized colloidal gold nanoparticles onto the NH2+ ion implantation-modified indium tin oxide *** scanning electron microscopy and electrochemical techniques,the as-prepared AuNPs attached NH2+ ion implantation-modified indium tin oxide electrode was characterized and compared with bare indium tin oxide *** a [Fe(CN)6]3 /[Fe(CN)6]4 redox probe,the increasingly facile heterogeneous electron transfer kinetics resulting from the attached gold nanoparticle arrays was *** gold nanoparticle arrays exhibited high catalytic activity toward the electro-oxidation of nitric oxide,which could provide electroanalytical application for nitric oxide sensing.

关键词： ion implantation gold nanoparticles indium tin oxide amino groups electrode

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Calculation of electron wave functions and refractive index of Ne

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Science china(Physics,Mechanics & Astronomy) 2008年第10期51卷 1489-1495页

作者： ZHU Min liu Wei ZHANG Tao key {1. of beam technology and material modification of ministry of education in beijing normal university Institute of Low Energy Nuclear PhysicsBeijing Radiation CenterBeijing 100875China

The radial wave functions of inner electron shell and outer electron shell of a Ne atom were obtained by the approximate analytical method and tested by calculating the ground state energy of the Ne atom. The equivalent volume of electron cloud and the refractive index of Ne were calculated. The calculated refractive index agrees well with the experimental result. Relationship between the refractive index and the wave function of Ne was discovered.

关键词： electron cloud refractive index density function theory (DFT) Slater radial wave function (STO) variation calculus

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Amplitude analysis of the decays D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)

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Chinese Physics C 2024年第8期48卷 6-33页

作者： M.Ablikim M.N.Achasov P.Adlarson O.Afedulidis X.C.Ai R.Aliberti A.Amoroso Q.An Y.Bai O.Bakina I.Balossino Y.Ban H.-R.bao V.Batozskaya K.Begzsuren N.Berger M.Berlowski M.Bertani D.Bettoni F.Bianchi E.Bianco A.Bortone I.Boyko R.A.Briere A.Brueggemann H.Cai X.Cai A.Calcaterra G.F.Cao N.Cao S.A.Cetin J.F.Chang W.L.Chang G.R.Che G.Chelkov C.Chen C.H.Chen Chao Chen G.Chen H.S.Chen M.L.Chen S.J.Chen S.L.Chen S.M.Chen T.Chen X.R.Chen X.T.Chen Y.B.Chen Y.Q.Chen Z.J.Chen Z.Y.Chen S.K.Choi X.Chu G.Cibinetto F.Cossio J.J.Cui H.L.Dai J.P.Dai A.Dbeyssi R.E.de Boer D.Dedovich C.Q.Deng Z.Y.Deng A.Denig I.Denysenko M.Destefanis F.De Mori B.Fang S.S.Fang W.X.Fang Y.Fang Y.Q.Fang R.Farinelli L.Fava F.Feldbauer G.Felici C.Q.Feng J.H.Feng Y.T.Feng K.Fischer M.Fritsch C.D.Fu J.L.Fu Y.W.Fu H.Gao Y.N.Gao Yang Gao S.Garbolino I.Garzia P.T.Ge Z.W.Ge C.Geng E.M.Gersabeck B.Ding X.X.Ding Y.Ding Y.Ding J.Dong L.Y.Dong M.Y.Dong X.Dong M.C.Du S.X.Du Z.H.Duan P.Egorov Y.H.Fan J.Fang JA.Gilman K.Goetzen L.Gong W.X.Gong W.Gradl S.Gramigna M.Greco M.H.Gu Y.T.Gu C.Y.Guan Z.L.Guan A.Q.Guo L.B.Guo M.J.Guo R.P.Guo Y.P.Guo A.Guskov J.Gutierrez K.L.Han T.T.Han X.Q.Hao F.A.Harris K.K.He K.L.He F.H.Heinsius C.H.Heinz Y.K.Heng C.Herold T.Holtmann P.C.Hong G.Y.Hou X.T.Hou Y.R.Hou Z.L.Hou B.Y.Hu H.M.Hu J.F.Hu T.Hu Y.Hu G.S.Huang K.X.Huang L.Q.Huang X.T.Huang Y.P.Huang T.Hussain F.H\"olzken N.H\"usken N.in der Wiesche M.Irshad J.Jackson S.Janchiv J.H.Jeong Q.Ji Q.P.Ji W.Ji X.B.Ji X.L.Ji Y.Y.Ji X.Q.Jia Z.K.Jia D.Jiang H.B.Jiang P.C.Jiang S.S.Jiang T.J.Jiang X.S.Jiang Y.Jiang J.B.Jiao J.K.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing X.M.Jing T.Johansson S.Kabana N.Kalantar-Nayestanaki X.L.Kang X.S.Kang M.Kavatsyuk B.C.Ke V.Khachatryan A.Khoukaz R.Kiuchi O.B.Kolcu B.Kopf M.Kuessner X.Kui A.Kupsc W.K\"uhn J.J.Lane P.Larin L.Lavezzi T.T.Lei Z.H.Lei H.Leithoff M.Lellmann T.Lenz C.Li C.Li C.H.Li Cheng Li D.M.Li F.Li G.Li H.Li H.B.Li H.J.Li H.N.Li Hui Li J.R.Li J.S.Li K.Li L.J.Li L.K.Li Lei Li M.H.Li P.R.Li Q.M.Li Q.X.Li R.Li S.X.Li T.Li W.D.Li W.G.Li X.Li X.H.Li X.L.Li X.Y.Li Y Institute of High Energy Physics Chinese Academy of SciencesBeijing 100049China Beihang university Beijing 100191China Bochum Ruhr-university D-44780 BochumGermany Budker Institute of Nuclear Physics SB RAS(BINP) Novosibirsk 630090Russia Carnegie Mellon university PittsburghPennsylvania 15213USA Central china {1. university Wuhan 430079China Central South university Changsha 410083China china Center of Advanced Science and {1. Beijing 100190China china {1. of Geosciences Wuhan 430074China Chung-Ang university Seoul06974Republic of Korea COMSATS university Islamabad Lahore CampusDefence RoadOff Raiwind Road54000 LahorePakistan Fudan university Shanghai 200433China GSI Helmholtzcentre for Heavy Ion Research GmbH D-64291 DarmstadtGermany Guangxi normal {1. Guilin 541004China Guangxi university Nanning 530004China Hangzhou normal {1. Hangzhou 310036China Hebei university Baoding 071002China Helmholtz Institute Mainz Staudinger Weg 18D-55099 MainzGermany Henan normal {1. Xinxiang 453007China Henan university Kaifeng 475004China Henan university of Science and {1. Luoyang 471003China Henan university of {1. Zhengzhou 450001China Huangshan College Huangshan 245000China Hunan normal {1. Changsha 410081China Hunan university Changsha 410082China Indian Institute of technology Madras Chennai 600036India Indiana university BloomingtonIndiana 47405USA INFN Laboratori Nazionali di Frascati INFN Laboratori Nazionali di FrascatiI-00044FrascatiItaly INFN Laboratori Nazionali di Frascati INFN Sezione di PerugiaI-06100PerugiaItaly INFN Laboratori Nazionali di Frascati University of PerugiaI-06100PerugiaItaly INFN Sezione di Ferrara INFN Sezione di FerraraI-44122FerraraItaly INFN Sezione di Ferrara University of FerraraI-44122FerraraItaly Inner Mongolia university Hohhot 010021China Institute of Modern Physics Lanzhou 730000China Institute of Physics and technology Peace Avenue 54BUlaanbaatar 13330Mongolia Instituto de A

Using e^(+)e^(−)annihilation data corresponding to an integrated luminosity of 2.93 fb^(−1.taken at the center-of-mass energy√s=3.773 GeV with the BESIII detector,a joint amplitude analysis is performed on the decays D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η).The fit fractions of individual components are obtained,and large interferences among the dominant components of the decays D^(0)→a_(1.(1.60)π,D^(0)→π(1.00)π,D^(0)→ρ(770)ρ(770),and D^(0)→2(ππ)_(S)are observed in both *** the obtained amplitude model,the CP-even fractions of D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η)are determined to be(75.2±1.1.(stat).±1.5_(syst.))%and(68.9±1.5_(stat).±2.4_(syst.))%,*** branching fractions of D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η)are measured to be(0.688±0.01._(stat.)±0.01._(syst.))%and(0.951.0.025_(stat.)±0.021.(syst.))%,*** amplitude analysis provides an important model for the binning strategy in measuring the strong phase parameters of D^(0)→4πwhen used to determine the CKM angleγ(ϕ_(3))via the B^(−)→DK^(−)decay.

关键词： BESIII D^(0)meson decays amplitude analysis CP-even fraction

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Internal magnetic-field-enhanced photogenerated charge separation in ferromagnetic TiO_(2)surface heterojunctions

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Journal of materials Science & {1. 2023年第29期160卷 240-247页

作者： Guojing Wang Shirong Xiong Yonghui Chen Chunchang Wang Shasha Lv Ke Jia Yunjie Xiang Jianbo liu Chong liu Zhengcao Li School of materials and Energy Lanzhou UniversityLanzhou 730000China State key {1. of New Ceramics and Fine Processing Key Laboratory of Advanced Materials(MOE)School of Materials Science and EngineeringTsinghua UniversityBeijing 100084China laboratory of Dielectric Functional {1.s School of Physics and Material ScienceAnhui UniversityHefei 230601China key {1. of beam technology Ministry of EducationCollege of Nuclear Science and TechnologyBeijing Normal UniversityBeijing 100875China School of materials and Energy Southwest UniversityChongqing 404100China

The use of the internal magnetic field of ferromagnets can effectively promote charge separation and transfer(CST)in photoelectrochemical energy ***,photoelectrochemical materials with a ferromagnetic field are scarce,and the internal magnetic field is negligible in nonferromagnetic *** address this issue,we propose a rational method for preparing ferromagnetic TiO_(2)powder using controllable oxygen vacancies in anatase TiO_(2)with co-exposed{001}and{101}***,an ex-cellent saturation magnetisation of 0.0014 emu/g in TiO_(2)is achieved owing to an asymmetric and uneven charge *** with that of nonferromagnetic TiO_(2),the efficiency of photocatalytic hydro-gen generation of ferromagnetic TiO_(2)is improved by 0.64 *** enhancement of photocatalytic hy-drogen generation is due to the different forces exerted on the electrons and holes in the magnetic field,which significantly improve the photogenerated CST efficiency of ferromagnetic TiO_(2).This result high-lights the significant role of the synergistic regulation of the crystal structure and defects in regulating the ferromagnetic characteristics of *** findings of this study provide guidance for leveraging point defects to promote CST for high-efficiency solar-energy conversion systems.

关键词： Photocatalysis TiO_(2){001}-{101}surface heterojunctions Oxygen vacancies Ferromagnetic

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制备工艺参量对超大颗粒石墨/铜基复合材料基本性能的影响

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真空科学与技术学报 2024年第4期44卷 332-340页

作者：张铭君程伟刘培生宋帅程瑜扬李翔宇北京师范大学射线束技术教育部重点实验室北京100875

添加超大石墨颗粒来提高铜的润滑性能具有制备操作简便、工艺成本低等优点。文章在研制超大粒度石墨颗粒作为功能相的铜基复合材料基础上,探讨制备工艺参量对该复合材料热导率、压缩强度和摩擦系数等基本性能的影响。研究发现,该复合制... 详细信息

添加超大石墨颗粒来提高铜的润滑性能具有制备操作简便、工艺成本低等优点。文章在研制超大粒度石墨颗粒作为功能相的铜基复合材料基础上,探讨制备工艺参量对该复合材料热导率、压缩强度和摩擦系数等基本性能的影响。研究发现,该复合制品的热导率明显大于采用等质量的较小粒度石墨原料的复合制品;石墨含量越多,颗粒越小,铜/石墨复合样品的热导率就越低。结果表明,该复合制品的规定非比例压缩强度和抗压强度均明显高于采用较小石墨颗粒的复合制品,其力学性能主要与石墨颗粒大小和添加量有关。在本工作的粒度范围(1.0~1.00μm)和含量范围(5%~1.%)内,石墨颗粒越大,含量越少,其复合制品的力学强度就越好。研究还表明:该复合制品的摩擦系数与采用等质量的较小粒度石墨原料的复合制品基本相当;对于摩擦性能,本工作中的石墨含量以1.%为佳,粒度以32目即约为720μm为佳。

关键词：铜基复合材料铜/石墨复合材料热导率压缩强度摩擦系数

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