{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"使用CF4和CH4为源气体,利用射频等离子体增强化学气相沉积法,制备了a-C:<span style=\"color:red\">F</span>:<span style=\"color:red\">H</span>薄膜样品.采用拉曼光谱仪、傅里叶变换红外光谱仪、X射线光电子能谱仪(XPS)对薄膜的结构进行了测试和分析.研究发现:该膜呈空间网状结构,膜内碳与氟、氢的结合主要以sp3形式存在,而sp2形式的含量相对较少;在薄膜内主要含有C-Fx(x=1,2,3)、C-C、C-<span style=\"color:red\">H</span>2、C-<span style=\"color:red\">H</span>3等以及不饱和C=C化学键;同时,薄膜中C-C-<span style=\"color:red\">F</span>键的含量比C-C-<span style=\"color:red\">F</span>2键的含量要高.在不同功率下沉积的薄膜,其化学键结构明显不同.","authors":[{"authorName":"肖剑荣","id":"d5cd55db-51af-4ffa-b77d-07107d4a1f1e","originalAuthorName":"肖剑荣"},{"authorName":"徐慧","id":"60319c7e-bd44-4025-a8e8-4a1e97a3c6e5","originalAuthorName":"徐慧"},{"authorName":"李幼真","id":"2edd9417-5be2-49dd-b6b7-5f4638075b40","originalAuthorName":"李幼真"},{"authorName":"刘雄飞","id":"650ab986-5ceb-47a8-8173-da3ed793a8a8","originalAuthorName":"刘雄飞"},{"authorName":"马松山","id":"4a9ab7f8-6350-46a2-b9be-a5f4fb4039a0","originalAuthorName":"马松山"},{"authorName":"简献忠","id":"5545c2c7-a30a-4878-bb1e-c34f27a89821","originalAuthorName":"简献忠"}],"doi":"","fpage":"1589","id":"9b1c35bd-9a0c-4de8-9d8c-dd65e137d126","issue":"10","journal":{"abbrevTitle":"ZGYSJSXB","coverImgSrc":"journal/img/cover/ZGYSJSXB.jpg","id":"88","issnPpub":"1004-0609","publisherId":"ZGYSJSXB","title":"中国有色金属学报"},"keywords":[{"id":"9de0974a-e422-475d-b659-1306cfd750ba","keyword":"a-C:<span style=\"color:red\">F</span>:<span style=\"color:red\">H</span>薄膜","originalKeyword":"a-C:F:H薄膜"},{"id":"c639f279-5f57-4ecb-a474-90fa77c422c7","keyword":"等离子体增强化学气相沉积","originalKeyword":"等离子体增强化学气相沉积"},{"id":"8b7f1713-4a68-4f1b-9f89-e7b8a9855cd1","keyword":"低介电常数","originalKeyword":"低介电常数"},{"id":"e0923a9a-98ee-416b-b7d7-cd2966341032","keyword":"化学键","originalKeyword":"化学键"}],"language":"zh","publisherId":"zgysjsxb200510019","title":"a-C:<span style=\"color:red\">F</span>:<span style=\"color:red\">H</span>薄膜的化学键结构","volume":"15","year":"2005"},{"abstractinfo":"描述了掺氧族离子(O2-,S2-,Se2-)NaCl晶体中(<span style=\"color:red\">F</span>+2)<span style=\"color:red\">H</span>心的制备过程,报道了氧族离子稳定的(<span style=\"color:red\">F</span>+2)<span style=\"color:red\">H</span>心的吸收光谱和发射光谱,测量了这些(<span style=\"color:red\">F</span>+2)<span style=\"color:red\">H</span>心的室温避光稳定性.研究表明,氧族离子对<span style=\"color:red\">F</span>+2心的稳定作用顺序为O2-＜Se2-＜S2-,而受这三种离子扰动的(<span style=\"color:red\">F</span>+2)<span style=\"color:red\">H</span>心的光谱峰位相对于纯<span style=\"color:red\">F</span>+2心的移动大小亦为这一顺序.这一顺序与它们相应元素的电子亲合能顺序相同(分别为1.47,2.02,2.07eV).从而,纠正了根据离子大小为预测的结果O2-＜S2-＜Se2-.本文结果对(<span style=\"color:red\">F</span>+2)<span style=\"color:red\">H</span>色心激光晶体材料的研究具有指导意义.研究还表明,随着离子半经的增大,生长出优质的掺杂晶体越来越困难.","authors":[{"authorName":"林碧洲","id":"56194798-e799-4f86-aa2e-7d26cf9d8991","originalAuthorName":"林碧洲"},{"authorName":"许承晃","id":"5a3820d4-a5e8-4de0-a4f5-cbb1a89b4bda","originalAuthorName":"许承晃"},{"authorName":"吴季怀","id":"c15fef71-4c9a-43a5-a460-e50b04919a4d","originalAuthorName":"吴季怀"},{"authorName":"邱继晨","id":"0f8a973b-36b5-40d8-ab13-094f43e27018","originalAuthorName":"邱继晨"}],"doi":"10.3969/j.issn.1000-985X.1998.01.022","fpage":"104","id":"6c9a9f24-a7e0-4d26-a5f9-b41b97630891","issue":"1","journal":{"abbrevTitle":"RGJTXB","coverImgSrc":"journal/img/cover/RGJTXB.jpg","id":"57","issnPpub":"1000-985X","publisherId":"RGJTXB","title":"人工晶体学报"},"keywords":[{"id":"3e465451-9ecb-4eb0-a3ca-c0d0122dd9b3","keyword":"色心激光","originalKeyword":"色心激光"},{"id":"e02574cf-b4ab-484f-91e5-a990d47e90a8","keyword":"激活心","originalKeyword":"激活心"},{"id":"2bdce156-7938-4c2a-b22f-4bf2467d5f5f","keyword":"掺杂效应","originalKeyword":"掺杂效应"},{"id":"771b0ca1-0f4b-43c2-b211-f258beb4e58c","keyword":"稳定性","originalKeyword":"稳定性"}],"language":"zh","publisherId":"rgjtxb98199801022","title":"NaCl晶体中氧族离子稳定的(<span style=\"color:red\">F</span>+2)<span style=\"color:red\">H</span>心","volume":"27","year":"1998"},{"abstractinfo":"The spin-Hamiltonian parameters (g factors g(parallel to), g(perpendicular to) and hyperfine structure constants (161)A(parallel to), (161)A(perpendicular to), (163)A(parallel to), (163)A(perpendicular to)) for Dy(3+) at the tetragonal <span style=\"color:red\">H</span>(<span style=\"color:red\">f</span>)(4+) site of <span style=\"color:red\">H</span>(<span style=\"color:red\">f</span>)SiO(4) crystal are calculated from the diagonalization (of energy matrix) method. In the method, we add the Zeeman (or magnetic) and hyperfine interaction terms to the conventional Hamiltonian used in the calculations of crystal-field energy levels. The 66 X 66 energy matrix concerning the new Hamiltonian is established by considering the ground multiplet (6)<span style=\"color:red\">H</span>(15/2) and the first to fifth excited multiplets (6)<span style=\"color:red\">H</span>(J) (where J=13/2, 11/2,9/2, 7/2 and 5/2), and the crystal-field parameters in the energy matrix are calculated from the superposition model. From the calculations, the spin-Hamiltonian parameters of <span style=\"color:red\">H</span>(<span style=\"color:red\">f</span>)SiO(4):Dy(3+) are explained reasonably and the signs of hyperfine structure constants for (161)Dy(3+) and (161)Dy(3+) isotopes in <span style=\"color:red\">H</span>(<span style=\"color:red\">f</span>)SiO(4) are suggested. The results are discussed. (C) 2010 Elsevier B.V. All rights reserved.","authors":[],"categoryName":"|","doi":"","fpage":"2697","id":"1eb3612c-e001-4d47-a927-ab37f91a46fb","issue":"12","journal":{"abbrevTitle":"PBM","id":"b1289047-807c-4b57-bffc-a126ac2ffa2a","issnPpub":"0921-4526","publisherId":"PBM","title":"Physica B-Condensed Matter"},"keywords":[{"id":"60a87cd6-594e-4d5e-ab30-c0732c50fa1c","keyword":"Electron paramagnetic resonance;Crystal-field theory;Point defect;Dy(3+);<span style=\"color:red\">H</span>(<span style=\"color:red\">f</span>)SiO(4);superposition-model analysis;single-crystals;paramagnetic-resonance;structure silicates;zircon;growth;hafnon;field;epr;er3","originalKeyword":"Electron paramagnetic resonance;Crystal-field theory;Point defect;Dy(3+);H(f)SiO(4);superposition-model analysis;single-crystals;paramagnetic-resonance;structure silicates;zircon;growth;hafnon;field;epr;er3"}],"language":"en","publisherId":"0921-4526_2010_12_1","title":"Theoretical calculations of the spin-Hamiltonian parameters for the tetragonal Dy(3+) center in <span style=\"color:red\">H</span>(<span style=\"color:red\">f</span>)SiO(4) crystal","volume":"405","year":"2010"},{"abstractinfo":"The surface segregation of substrate elements through the Au layer in the Au-Ni-Kovar sys- tem specimens heated at 250—350℃ for 0.5—1.5 <span style=\"color:red\">h</span> has been studied by <span style=\"color:red\">SAM</span> and XPS. Visual evidence of the mechanism for Ni and Co surface segregation of the complicated sys- tem has been given,i.e.Ni and Co penetrated the gold layer mainly by grain boundary diffu- sion and then covered the Au layer by surface diffusion.The strdy results of the chemical states of surface segregation elements not only indicate that oxygen adsorption and oxidation reaction are the driving force for the surface segregation of Ni and Co,but also show that the above segregation can result in water absorption on surfaces.","authors":[{"authorName":"QI Yunxin TANG Wentai XIA Jianguo Nei Mongol Institute of Metallic Materials","id":"b0ffdb2c-e6ff-4e95-91d1-d478d87559f9","originalAuthorName":"QI Yunxin TANG Wentai XIA Jianguo Nei Mongol Institute of Metallic Materials"},{"authorName":"Baotou","id":"186a2cde-c0d7-4322-ac8b-b4ac7a3d09e3","originalAuthorName":"Baotou"},{"authorName":"ChinaLI Wang ZHAN Zhenzong Institute of Physical and Chemical Engineering Research","id":"8f73b234-5119-4f77-9711-8d70c2e7304b","originalAuthorName":"ChinaLI Wang ZHAN Zhenzong Institute of Physical and Chemical Engineering Research"},{"authorName":"Tianjin","id":"966a5da1-5599-4870-a184-c093db926846","originalAuthorName":"Tianjin"},{"authorName":"China","id":"c5031cf6-051b-465b-8b12-972a7e12a9b8","originalAuthorName":"China"}],"categoryName":"|","doi":"","fpage":"219","id":"399e571b-e879-4ddb-8d94-beca28f88b3d","issue":"9","journal":{"abbrevTitle":"JSXBYWB","coverImgSrc":"journal/img/cover/amse.jpg","id":"49","issnPpub":"1006-7191","publisherId":"JSXBYWB","title":"金属学报(英文版)"},"keywords":[{"id":"0874d2b5-172f-494e-b565-e230c3ded70f","keyword":"Au-Ni-Kovar alloy system","originalKeyword":"Au-Ni-Kovar alloy system"},{"id":"1e332b08-77e7-4fd9-a83f-cd0c888c2e31","keyword":"null","originalKeyword":"null"},{"id":"00a6ee0b-9565-420a-8950-77c386f128a3","keyword":"null","originalKeyword":"null"},{"id":"04cf2acd-c8bd-4588-83fc-db5cf28de304","keyword":"null","originalKeyword":"null"},{"id":"bde1b2d7-dfad-488b-bde6-8c28eda8f300","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1006-7191_1991_9_13","title":"<span style=\"color:red\">SAM</span> AND XPS STUDIES ON SURFACE SEGREGATION OF SUBSTRATE ELEMENTS IN Au-Ni-KOVAR ALLOY SYSTEM","volume":"4","year":"1991"},{"abstractinfo":"本文采用<span style=\"color:red\">SAM</span>和XPS对实用Au-Ni-Kovar合金系统热处理样品(250—350℃,0.5—1.5<span style=\"color:red\">h</span>)进行了基底元素穿透Au层的表面偏聚研究,给出了这一复杂系统中Ni,Co表面偏聚机理的直观证据,即Ni,Co主要是通过晶界扩散穿透Au层而后以表面扩散覆盖镀Au表面的;表面偏聚元素化学态的研究则不仅表明,氧的吸附和氧化反应是Ni,Co表面偏聚的驱动力,而且发现,上述偏聚会引起样品表面吸水的现象。","authors":[{"authorName":"齐芸馨","id":"91c0f28f-06b5-46a0-be82-795921dd6fb4","originalAuthorName":"齐芸馨"},{"authorName":"唐文泰","id":"0db2fe85-c312-4020-a787-3f7ec744f6e1","originalAuthorName":"唐文泰"},{"authorName":"夏建国","id":"e205da5f-fc00-487c-b517-8e184e8f502b","originalAuthorName":"夏建国"},{"authorName":"李望","id":"9d92c82a-4457-4582-9e15-5c7c15afa548","originalAuthorName":"李望"},{"authorName":"展振宗","id":"cc86d657-8846-4004-81d5-ee1884ffbb9b","originalAuthorName":"展振宗"}],"categoryName":"|","doi":"","fpage":"145","id":"6bf2e3af-52bc-4982-92b4-5e9e81b27199","issue":"6","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"4d4a724b-ccfc-4fc7-8021-77cb2876292b","keyword":"Au-Ni-Kovar合金系统","originalKeyword":"Au-Ni-Kovar合金系统"},{"id":"541f7a49-24ea-420c-9853-152bdbf8d84e","keyword":"surface segregation","originalKeyword":"surface segregation"},{"id":"7e4fb007-f0bf-48c1-8ade-355fa4a8a902","keyword":"substrate element","originalKeyword":"substrate element"},{"id":"bcb6fa4f-4578-4134-9a59-b064b54363e7","keyword":"<span style=\"color:red\">SAM</span>","originalKeyword":"SAM"},{"id":"73ae95aa-f7f1-4455-961c-e1bf92a0e732","keyword":"XPS","originalKeyword":"XPS"}],"language":"zh","publisherId":"0412-1961_1990_6_30","title":"Au-Ni-Kovar合金系统基底元素表面偏聚的<span style=\"color:red\">SAM</span>和XPS研究","volume":"26","year":"1990"},{"abstractinfo":"采用循环伏安法和线性扫描技术等电化学研究方法，系统研究了电解液体系中各阴阳离子对锑电沉积过程的影响。通过测定Sb3＋、NH4＋、<span style=\"color:red\">F</span>-、SO2-4及草酸等组分不同质量浓度下体系的循环伏安曲线、稳态极化曲线及塔菲尔曲线，分析了各离子在电解过程中的电化学行为及作用，确定了<span style=\"color:red\">H</span>2 SO4-NH4 <span style=\"color:red\">F</span>-SbF3电解液体系合适的成分为Sb3＋90～120 g／L、NH4＋50 g／L、<span style=\"color:red\">F</span>-80 g／L、<span style=\"color:red\">H</span>2 SO4360 g／L、<span style=\"color:red\">H</span>2 C2 O44～10 g／L。在此电解液体系下进行了粗锑的电解精炼试验，阴极锑纯度为99．9436％，达到国标1号精锑标准，阴极电流效率为97．60％。","authors":[{"authorName":"崔焱","id":"d5ec0310-1f0d-41be-8c7b-c36ba6b719b5","originalAuthorName":"崔焱"},{"authorName":"林艳","id":"52e1da36-0d40-4232-bd13-b80c70bfeab9","originalAuthorName":"林艳"},{"authorName":"谢刚","id":"847e0154-eb2c-4430-af1b-51cb44d1f47e","originalAuthorName":"谢刚"},{"authorName":"杨大锦","id":"4c9b0078-0748-41e0-922f-fcee25283706","originalAuthorName":"杨大锦"}],"doi":"10.11792/hj20140412","fpage":"50","id":"141a67f4-dc9e-46e5-b47d-73b4fa7b210e","issue":"4","journal":{"abbrevTitle":"HJ","coverImgSrc":"journal/img/cover/HJ.jpg","id":"44","issnPpub":"1001-1277","publisherId":"HJ","title":"黄金"},"keywords":[{"id":"3b244a1f-0ad8-4042-9043-f9ae2ff422e9","keyword":"锑","originalKeyword":"锑"},{"id":"a37202bf-9531-4909-9d67-1712554f7186","keyword":"电解精炼","originalKeyword":"电解精炼"},{"id":"de556e37-7b76-4f24-974a-7f3caae3bb3c","keyword":"<span style=\"color:red\">H</span>2 SO4 -NH4 <span style=\"color:red\">F</span>-SbF3体系","originalKeyword":"H2 SO4 -NH4 F-SbF3体系"}],"language":"zh","publisherId":"huangj201404014","title":"<span style=\"color:red\">H</span>2 SO4-NH4 <span style=\"color:red\">F</span>-SbF3粗锑电解精炼体系研究","volume":"","year":"2014"},{"abstractinfo":"改变CHF3/CH4流量比R=[CHF3]/([CHF3]+[CH4]),采用微波电子回旋共振等离子体化学气相沉积(MWECR-CVD)方法沉积a-C:<span style=\"color:red\">F</span>:<span style=\"color:red\">H</span>薄膜.a-C:<span style=\"color:red\">F</span>:<span style=\"color:red\">H</span>薄膜的结构和光学带隙使用傅立叶变换红外光谱和紫外-可见光谱来表征.红外结果表明,在低流量比R(R<64%)下,薄膜的红外特征结构主要以-CF(1060cm-1),-CF2(1120cm-1)以及-CHx(2800～3000cm-1)的伸缩振动为主;在高流量比R(R＞64%)下,薄膜表现为类聚四氟乙烯(PTFE)的结构特征,典型的红外特征峰是位于1220cm-1处的-CF2反对称伸缩振动.薄膜的光学带隙Eg随流量比R的变化表现为先降后升.进一步研究表明,薄膜中的<span style=\"color:red\">H</span>和<span style=\"color:red\">F</span>浓度调制着薄膜的 C==C共轭双键结构,使光学带隙Eg从2.37到3.3之间变化.","authors":[{"authorName":"甘肇强","id":"cb1d1c62-0de3-432c-9405-adfb25d47c5e","originalAuthorName":"甘肇强"},{"authorName":"陆新华","id":"e8848122-0260-451e-bc6f-74e795883657","originalAuthorName":"陆新华"}],"doi":"10.3969/j.issn.1673-2812.2002.02.004","fpage":"163","id":"104d11ef-b95e-462c-be35-56ece6cd4c01","issue":"2","journal":{"abbrevTitle":"CLKXYGCXB","coverImgSrc":"journal/img/cover/CLKXYGCXB.jpg","id":"13","issnPpub":"1673-2812","publisherId":"CLKXYGCXB","title":"材料科学与工程学报"},"keywords":[{"id":"4f60bda5-9a22-477b-a50b-12ab21b38f29","keyword":"a-C:<span style=\"color:red\">F</span>:<span style=\"color:red\">H</span>薄膜","originalKeyword":"a-C:F:H薄膜"},{"id":"2173e3d8-6579-4d25-bd14-21bef8ad3a4c","keyword":"傅立叶变换红外光谱","originalKeyword":"傅立叶变换红外光谱"},{"id":"8dedf348-1663-4de5-8ae3-036fbf20e604","keyword":"紫外可见光谱","originalKeyword":"紫外可见光谱"}],"language":"zh","publisherId":"clkxygc200202004","title":"微波ECR-CVD法制备a-C:<span style=\"color:red\">F</span>:<span style=\"color:red\">H</span>膜的红外吸收及其光学带隙","volume":"20","year":"2002"},{"abstractinfo":"The variation of carbon composition in undercooled austenite during bainitic incubation period has been investigated in 40CrMnSiMoVA by scanning auger microprobe (<span style=\"color:red\">SAM</span>). The results show that the outstanding diffusion and redistribution of carbon occur in isothermally reacted specimens. This leads to the formation of carbon-poor regions (CPR) near austenite grain boundaries and in austenite grains. The carbon content in CPR exceeds the equilibrium carbon composition of ferrite. Furthermore, it is indicated that the existence of CPR is thermodynamically possible.","authors":[{"authorName":"Xiaolei WU","id":"0a464092-8733-4b40-beb3-f9ad2fdf5980","originalAuthorName":"Xiaolei WU"},{"authorName":"Husheng JIA","id":"0230b2ab-0707-458a-875d-4cb545c8a511","originalAuthorName":"Husheng JIA"},{"authorName":"Xiyan ZHANG and Mokuang KANG(Dept. of Materials Science & Engineering","id":"a1896efa-0c0f-49b0-8cc5-b527cea61199","originalAuthorName":"Xiyan ZHANG and Mokuang KANG(Dept. of Materials Science & Engineering"},{"authorName":" Northwestern Polytechnical University","id":"88b96b70-825a-4752-9d1c-ab84f04da20d","originalAuthorName":" Northwestern Polytechnical University"},{"authorName":" Xi'an","id":"cfde7893-0168-4fc0-9e43-d7984208fd63","originalAuthorName":" Xi'an"},{"authorName":" 710072","id":"dc724825-09cd-4a90-abaa-bee78edb6038","originalAuthorName":" 710072"},{"authorName":" China)(To whom correspondence should be addressed)","id":"98c5384a-f7f9-483f-8027-ca425c45fe59","originalAuthorName":" China)(To whom correspondence should be addressed)"}],"categoryName":"|","doi":"","fpage":"353","id":"3bac58cc-f72b-4246-8208-6cf06f1cedfb","issue":"5","journal":{"abbrevTitle":"CLKXJSY","coverImgSrc":"journal/img/cover/JMST.jpg","id":"11","issnPpub":"1005-0302 ","publisherId":"CLKXJSY","title":"材料科学技术（英文）"},"keywords":[],"language":"en","publisherId":"1005-0302_1995_5_7","title":"Study of Carbon-poor Regions of Austenite during Bainitic Incubation Period by <span style=\"color:red\">SAM</span>","volume":"11","year":"1995"},{"abstractinfo":"通过对已累积运行15万<span style=\"color:red\">h</span>后<span style=\"color:red\">F</span>12钢主蒸汽管道取样弯管的持久强度以及高温蠕变裂纹开裂和扩展速率的试验研究,应用积累的<span style=\"color:red\">F</span>12钢高温持久性能数据,确定原始材料的Larson-Miller方程,并据此方程和弯管的持久性能数据,统计估算取样弯管的剩余寿命和等效运行应力;再应用高温蠕变裂纹开裂和扩展寿命评估法,计算取样弯管在等效运行应力条件下的高温蠕变裂纹开裂和扩展寿命,并对其进行剩余寿命评估;最后根据弯管的显微组织对预测结果进行了验证.结果表明:用Larson-Miller参数法评估得到的主蒸汽管道的剩余寿命为73 515 <span style=\"color:red\">h</span>,等效运行应力为103.97MPa;用蠕变裂纹开裂和扩展寿命评估法得到的剩余寿命为153 354 <span style=\"color:red\">h</span>;该主蒸汽管道仍可正常运行近10 a;预测结果与试验验证结果一致.","authors":[{"authorName":"黄维浩","id":"4b4249ce-e689-4359-b57f-794bad6b6d09","originalAuthorName":"黄维浩"},{"authorName":"张瑞","id":"b0246298-6846-44f5-971c-0a31dbb48940","originalAuthorName":"张瑞"},{"authorName":"唐松青","id":"16e66d4e-4ef6-46b6-aa63-d253ea98f59b","originalAuthorName":"唐松青"},{"authorName":"赵中平","id":"2a759e37-b1ee-47f3-8b9e-81292b10ff85","originalAuthorName":"赵中平"},{"authorName":"彭行金","id":"7ff13b06-c7dd-4194-a677-84a3b5540e0f","originalAuthorName":"彭行金"}],"doi":"","fpage":"90","id":"59ec0950-0565-4c88-8136-631ef9d3336d","issue":"1","journal":{"abbrevTitle":"JXGCCL","coverImgSrc":"journal/img/cover/JXGCCL.jpg","id":"45","issnPpub":"1000-3738","publisherId":"JXGCCL","title":"机械工程材料"},"keywords":[{"id":"04bb87cf-cc73-41a0-b0fa-6c4f5ea2b06c","keyword":"<span style=\"color:red\">F</span>12钢","originalKeyword":"F12钢"},{"id":"dee5183a-3758-4b64-be62-c683c4c3eb99","keyword":"主蒸汽管道","originalKeyword":"主蒸汽管道"},{"id":"a09a9f18-0427-4925-8276-fcae06a09b65","keyword":"持久性能","originalKeyword":"持久性能"},{"id":"52974a8f-d8f6-4ddc-ab80-d15e045f3510","keyword":"剩余寿命","originalKeyword":"剩余寿命"}],"language":"zh","publisherId":"jxgccl201401020","title":"运行15万<span style=\"color:red\">h</span>后<span style=\"color:red\">F</span>12钢主蒸汽管道剩余寿命的预测与试验验证","volume":"38","year":"2014"},{"abstractinfo":"探索研究了<span style=\"color:red\">F-8H</span>3/602芳纶织物增强树脂基复合材料层合板不同树脂含量对其冲击韧性、层间剪切强度及弯曲性能的影响,并采用显微镜及扫描电镜对破坏试样形貌进行观察.结果表明芳纶复合材料的树脂含量对其冲击韧性、层间剪切强度及弯曲性能影响较为明显,树脂含量为46.02wt％的芳纶复合材料层合板的0°冲击韧性为22 J/cm2、0°层间剪切强度为49.1 MPa、0°弯曲强度为506 MPa;在一定的树脂含量下,芳纶复合材料的0°冲击韧性、层间剪切强度及弯曲性能较90°的性能更优异;破坏试样的形貌表明纤维与树脂界面结合较为薄弱.","authors":[{"authorName":"易凯","id":"a9a51436-b14d-4704-84c1-172d39967ab9","originalAuthorName":"易凯"},{"authorName":"耿东兵","id":"52ddc9fb-5d44-428c-8bc0-787feec2ce64","originalAuthorName":"耿东兵"},{"authorName":"杨智勇","id":"982278a6-492d-4b5b-b8dc-f3bbd2adc989","originalAuthorName":"杨智勇"},{"authorName":"杨坚","id":"23b73da5-06b2-4bd3-8107-2509c062328b","originalAuthorName":"杨坚"},{"authorName":"贺晔红","id":"8a18c16f-db49-4034-bcc3-fe2cee23e9ac","originalAuthorName":"贺晔红"}],"doi":"10.3969/j.issn.1007-2330.2015.02.014","fpage":"59","id":"e8f21b20-718b-4269-bc2d-ebe12a3a00be","issue":"2","journal":{"abbrevTitle":"YHCLGY","coverImgSrc":"journal/img/cover/YHCLGY.jpg","id":"77","issnPpub":"1007-2330","publisherId":"YHCLGY","title":"宇航材料工艺   "},"keywords":[{"id":"1032a155-a36a-48dd-8d15-713b5103b0e8","keyword":"芳纶复合材料","originalKeyword":"芳纶复合材料"},{"id":"3a6da9bf-2745-4b49-b18d-7dbc66edf8f3","keyword":"树脂含量","originalKeyword":"树脂含量"},{"id":"f93ce103-f0bc-4f5e-a079-51b89a747495","keyword":"冲击韧性","originalKeyword":"冲击韧性"},{"id":"21a75137-738f-4d29-ab7d-00ef661989a5","keyword":"层间剪切强度","originalKeyword":"层间剪切强度"},{"id":"cafb3acb-9b4e-4dc3-8ff4-bfb0450c74ae","keyword":"弯曲性能","originalKeyword":"弯曲性能"}],"language":"zh","publisherId":"yhclgy201502014","title":"树脂含量对<span style=\"color:red\">F-8H</span>3/602芳纶复合材料性能的影响","volume":"45","year":"2015"}],"totalpage":3180,"totalrecord":31800}