{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"利用直流磁控溅射法在室温玻璃<span style=\"color:red\">衬底</span>上制备出了可见光透过率高、电阻率低<span style=\"color:red\">的</span>掺锆氧化锌(ZnO: Zr)透明导电薄膜.并系统地研究了<span style=\"color:red\">靶</span><span style=\"color:red\">与</span><span style=\"color:red\">衬底</span><span style=\"color:red\">之间</span><span style=\"color:red\">的</span><span style=\"color:red\">距离</span>对ZnO: Zr薄膜结构、形貌、光学及电学性能<span style=\"color:red\">的</span>影响.实验结果表明,<span style=\"color:red\">靶</span><span style=\"color:red\">与</span><span style=\"color:red\">衬底</span><span style=\"color:red\">之间</span><span style=\"color:red\">的</span><span style=\"color:red\">距离</span>对ZnO: Zr薄膜<span style=\"color:red\">的</span>生长速率、结晶质量及电学性能有很大影响,而对其光学性能影响不大.实验制备<span style=\"color:red\">的</span>ZnO: Zr为六方纤锌矿结构<span style=\"color:red\">的</span>多晶薄膜,且具有垂直于<span style=\"color:red\">衬底</span>方向<span style=\"color:red\">的</span>c轴择优取向.当<span style=\"color:red\">靶</span><span style=\"color:red\">与</span><span style=\"color:red\">衬底</span><span style=\"color:red\">之间</span><span style=\"color:red\">的</span><span style=\"color:red\">距离</span>从60 mm减小到50 mm时,薄膜<span style=\"color:red\">的</span>晶化程度提高、晶粒尺寸增大,薄膜<span style=\"color:red\">的</span>电阻率减小;然而,当<span style=\"color:red\">距离</span>继续减小时,薄膜<span style=\"color:red\">的</span>晶化程度降低、晶粒尺寸减小,薄膜<span style=\"color:red\">的</span>电阻率增大.当<span style=\"color:red\">靶</span><span style=\"color:red\">与</span><span style=\"color:red\">衬底</span><span style=\"color:red\">之间</span><span style=\"color:red\">的</span><span style=\"color:red\">距离</span>为50 mm时,薄膜<span style=\"color:red\">的</span>电阻率达到最小值4.2×10-4 Ω·cm,其可见光透过率超过95%.实验制备<span style=\"color:red\">的</span>ZnO: Zr薄膜可以用作薄膜太阳能电池和液晶显示器<span style=\"color:red\">的</span>透明电极.","authors":[{"authorName":"张化福","id":"f0c3d7e9-2373-4ac2-b0fb-8f54d1f0ee0d","originalAuthorName":"张化福"},{"authorName":"陈钦生","id":"ee8fbe21-4bd5-4535-b4ad-fa18124b05e7","originalAuthorName":"陈钦生"},{"authorName":"刘汉法","id":"4bccb806-393f-405b-9b62-b534d14a0596","originalAuthorName":"刘汉法"}],"doi":"","fpage":"1412","id":"b6492d2b-c056-4642-92fb-277bf0f33ef3","issue":"6","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":"b9f7f190-5152-475b-bb54-486ec6effc09","keyword":"<span style=\"color:red\">靶</span><span style=\"color:red\">与</span><span style=\"color:red\">衬底</span><span style=\"color:red\">之间</span><span style=\"color:red\">的</span><span style=\"color:red\">距离</span>","originalKeyword":"靶与衬底之间的距离"},{"id":"546f5ee1-9ef9-4202-a7f4-5fb372cb8a05","keyword":"ZnO:Zr","originalKeyword":"ZnO:Zr"},{"id":"45d49ae4-5776-4d9c-a327-0f1a01686d49","keyword":"透明导电薄膜","originalKeyword":"透明导电薄膜"},{"id":"17042be0-6632-4926-be3b-bffcf00af112","keyword":"磁控溅射","originalKeyword":"磁控溅射"}],"language":"zh","publisherId":"rgjtxb98201006013","title":"<span style=\"color:red\">靶</span><span style=\"color:red\">与</span><span style=\"color:red\">衬底</span><span style=\"color:red\">之间</span><span style=\"color:red\">的</span><span style=\"color:red\">距离</span>对ZnO:Zr透明导电薄膜性能<span style=\"color:red\">的</span>影响","volume":"39","year":"2010"},{"abstractinfo":"建设在同一路由内<span style=\"color:red\">的</span>管道和高压交流输电线,管道不可避免地受到高压交流输电线<span style=\"color:red\">的</span>干扰,而管道<span style=\"color:red\">与</span>高压线<span style=\"color:red\">之间</span><span style=\"color:red\">的</span>安全<span style=\"color:red\">距离</span>则是保证管道不必采取排流<span style=\"color:red\">的</span>重要指标.为探究埋地管道<span style=\"color:red\">与</span>高压交流输电线安全<span style=\"color:red\">距离</span><span style=\"color:red\">的</span>问题,分别取4,6,8,10V作为管道上感应电压<span style=\"color:red\">的</span>限值,利用相关软件研究了高压线稳态运行电流、管道<span style=\"color:red\">与</span>高压线<span style=\"color:red\">的</span>平行长度和土壤电阻率对安全<span style=\"color:red\">距离</span><span style=\"color:red\">的</span>影响规律.结果表明,把4V作为感应电压限值时,安全<span style=\"color:red\">距离</span>远大于其他三个限值对应<span style=\"color:red\">的</span>安全<span style=\"color:red\">距离</span>;随着平行长度、稳态运行电流和土壤电阻率<span style=\"color:red\">的</span>增大,安全<span style=\"color:red\">距离</span>也相应增大.","authors":[{"authorName":"杨超","id":"ce691ce8-7d3e-4349-9d9d-4461d8f46c94","originalAuthorName":"杨超"},{"authorName":"李自力","id":"1e5b2cc8-aed7-4f04-92ab-3cd97dce0a48","originalAuthorName":"李自力"},{"authorName":"崔淦","id":"7c01606c-ad08-4306-8e3e-d1d0773b8212","originalAuthorName":"崔淦"},{"authorName":"丁小勇","id":"c15e671a-8e41-41ad-a70a-ff8343e1180f","originalAuthorName":"丁小勇"}],"doi":"10.11973/fsyfh-201601013","fpage":"56","id":"07d01b21-67e9-41fe-8c29-b37f367eeadf","issue":"1","journal":{"abbrevTitle":"FSYFH","coverImgSrc":"journal/img/cover/FSYFH.jpg","id":"25","issnPpub":"1005-748X","publisherId":"FSYFH","title":"腐蚀与防护"},"keywords":[{"id":"de5c4d3d-0d88-40c2-8735-b5fa668dc093","keyword":"埋地管道","originalKeyword":"埋地管道"},{"id":"79ee3c57-92f3-4b27-a5b7-db9c960dc825","keyword":"高压交流输电线","originalKeyword":"高压交流输电线"},{"id":"10a9ca64-1d37-460a-88e9-73833f0657d5","keyword":"感应电压","originalKeyword":"感应电压"},{"id":"ec04e1cb-e4e2-4926-a045-1d420d490b0d","keyword":"安全<span style=\"color:red\">距离</span>","originalKeyword":"安全距离"}],"language":"zh","publisherId":"fsyfh201601013","title":"埋地管道<span style=\"color:red\">与</span>高压交流输电线<span style=\"color:red\">之间</span><span style=\"color:red\">的</span>安全<span style=\"color:red\">距离</span>","volume":"37","year":"2016"},{"abstractinfo":"实验利用直流和射频磁控溅射方法交替沉积Cu-SiO2纳米复合膜,研究不同Cu<span style=\"color:red\">靶</span>功率和<span style=\"color:red\">衬底</span>温度对纳米复合膜<span style=\"color:red\">的</span>相结构和光吸收性能<span style=\"color:red\">的</span>影响.结果表明:随着Cu<span style=\"color:red\">靶</span>功率<span style=\"color:red\">的</span>增加,金属Cu纳米颗粒尺寸增大,导致光吸收峰峰位发生红移;随着<span style=\"color:red\">衬底</span>温度<span style=\"color:red\">的</span>升高,由于Cu再蒸发效应致使金属Cu纳米颗粒尺寸减小,引起光吸收峰峰位发生蓝移;<span style=\"color:red\">与</span>室温下沉积态Cu-SiO2纳米复合膜相比,在<span style=\"color:red\">衬底</span>加热条件下沉积<span style=\"color:red\">的</span>纳米复合膜在可见光波段出现了明显<span style=\"color:red\">的</span>表面等离子体共振吸收峰.因此,Cu<span style=\"color:red\">靶</span>功率和<span style=\"color:red\">衬底</span>温度对Cu-SiO2纳米复合薄膜<span style=\"color:red\">的</span>结晶状况和光吸收性能有显著影响.","authors":[{"authorName":"赵志明","id":"8b38c0dd-f151-4389-b876-edf268966a03","originalAuthorName":"赵志明"},{"authorName":"邢少敏","id":"8088835b-ad65-4970-a456-b94ed70489fc","originalAuthorName":"邢少敏"},{"authorName":"张国君","id":"f0b79670-074c-4313-b1a9-8dc978a3bf24","originalAuthorName":"张国君"},{"authorName":"白力静","id":"92550d2c-8de4-4c38-8b82-73c8a22802f7","originalAuthorName":"白力静"}],"doi":"","fpage":"2539","id":"ed8b033d-3c76-4926-8280-7a81a68f1948","issue":"10","journal":{"abbrevTitle":"XYJSCLYGC","coverImgSrc":"journal/img/cover/XYJSCLYGC.jpg","id":"69","issnPpub":"1002-185X","publisherId":"XYJSCLYGC","title":"稀有金属材料与工程"},"keywords":[{"id":"c9110d73-1ab2-457c-a4c5-85710190e076","keyword":"Cu-SiO2纳米复合膜","originalKeyword":"Cu-SiO2纳米复合膜"},{"id":"60c0eea7-25e6-4323-8d03-e15456c95671","keyword":"磁控溅射","originalKeyword":"磁控溅射"},{"id":"5b8100f9-e9f3-4ce1-8115-ebe69ea1f319","keyword":"相结构","originalKeyword":"相结构"},{"id":"eb1ca0a9-faa8-43b9-8c28-8129421bd564","keyword":"光吸收性能","originalKeyword":"光吸收性能"}],"language":"zh","publisherId":"xyjsclygc201510039","title":"Cu<span style=\"color:red\">靶</span>功率和<span style=\"color:red\">衬底</span>温度对Cu-SiO2纳米复合膜<span style=\"color:red\">的</span>相结构<span style=\"color:red\">与</span>光吸收性能影响","volume":"44","year":"2015"},{"abstractinfo":"采用基于密度泛函理论框架下<span style=\"color:red\">的</span>第一性原理,研究石墨烯<span style=\"color:red\">与</span>Ge<span style=\"color:red\">衬底</span><span style=\"color:red\">之间</span><span style=\"color:red\">的</span>界面结构.计算结果表明,在3种<span style=\"color:red\">衬底</span>Ge(111)、Ge(100)和Ge(110)上界面结合能有相同<span style=\"color:red\">的</span>规律,均在平衡<span style=\"color:red\">距离</span>为3.3A时获得最低能量,平均每个碳原子<span style=\"color:red\">的</span>界面结合能分别为24.3 meV、21.1 meV和23.3 meV;通过构造0～60°<span style=\"color:red\">之间</span>不同<span style=\"color:red\">的</span>界面夹角,发现一个高对称性<span style=\"color:red\">的</span>界面结构;相比本征Ge<span style=\"color:red\">衬底</span>,石墨烯<span style=\"color:red\">与</span>H钝化后Ge<span style=\"color:red\">衬底</span><span style=\"color:red\">之间</span><span style=\"color:red\">的</span>界面平衡<span style=\"color:red\">距离</span>增大,结合能降低;H钝化能有效地屏蔽石墨烯<span style=\"color:red\">与</span>Ge<span style=\"color:red\">衬底</span><span style=\"color:red\">之间</span><span style=\"color:red\">的</span>相互作用,恢复了本征石墨烯<span style=\"color:red\">的</span>电子性质,起到缓冲层作用.","authors":[{"authorName":"史晓华","id":"a923e6a0-7631-4792-afcf-de115bf07876","originalAuthorName":"史晓华"},{"authorName":"王刚","id":"a1191ece-2093-4265-b843-4106b16a8cd4","originalAuthorName":"王刚"},{"authorName":"郭庆磊","id":"2bbd32cf-0928-4041-8fe9-203b62e5c317","originalAuthorName":"郭庆磊"},{"authorName":"张苗","id":"a36ff7a6-43e3-42a0-83d5-9b3c2d320a9d","originalAuthorName":"张苗"},{"authorName":"狄增峰","id":"012211f3-059b-4d5f-af4e-cae97da8011a","originalAuthorName":"狄增峰"}],"doi":"10.11896/j.issn.1005-023X.2015.10.032","fpage":"137","id":"1b9b7e90-123e-4071-aa29-f60541976417","issue":"10","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"72a7c0d7-0313-4321-8fd5-8e9925082bf8","keyword":"锗<span style=\"color:red\">衬底</span>","originalKeyword":"锗衬底"},{"id":"b2d1a4b4-c7c3-4689-a9f0-f5e4002be3ba","keyword":"石墨烯","originalKeyword":"石墨烯"},{"id":"a5c983f8-4bc4-491f-acef-951f1c10ab1e","keyword":"界面结构","originalKeyword":"界面结构"},{"id":"51706abe-d140-476e-a140-ff5968e621e8","keyword":"第一性原理","originalKeyword":"第一性原理"}],"language":"zh","publisherId":"cldb201510032","title":"石墨烯<span style=\"color:red\">与</span>锗<span style=\"color:red\">衬底</span>界面结构<span style=\"color:red\">的</span>第一性原理研究","volume":"29","year":"2015"},{"abstractinfo":"以硫化镉（CdS ）为主要原料，氯化镉（C dC l2）为助熔剂，采用干压成型、真空烧结<span style=\"color:red\">的</span>方式制备CdS陶瓷<span style=\"color:red\">靶</span>材。探讨了原料性质、烧结温度、CdCl2添加量对<span style=\"color:red\">靶</span>材相对密度、烧结线收缩率、显气孔率及表面电阻率<span style=\"color:red\">的</span>影响。用阿基米德法测定<span style=\"color:red\">靶</span>材密度、用四探针测试仪测试<span style=\"color:red\">靶</span>材表面电阻率、用X RD测试<span style=\"color:red\">靶</span>材晶相结构、用SEM 观察<span style=\"color:red\">靶</span>材微观形貌。实验结果表明，<span style=\"color:red\">靶</span>材试样<span style=\"color:red\">的</span>晶相主要为六方相CdS ，晶粒均匀（晶粒大小在3～8μm<span style=\"color:red\">之间</span>），密度达到45．5 g／cm3，显气孔率45．9％，表面电阻率892．Ω?cm ，能满足磁控溅射镀膜工艺对<span style=\"color:red\">靶</span>材<span style=\"color:red\">的</span>指标要求。","authors":[{"authorName":"董雪振","id":"4e518568-2bd4-4f87-ab5e-5975f4c7217c","originalAuthorName":"董雪振"},{"authorName":"吴任平","id":"2eee80c9-4138-4248-88c9-15fae896ec35","originalAuthorName":"吴任平"}],"doi":"10.3969/ji.ssn1.001-97312.0151.70.31","fpage":"17140","id":"57138212-375f-4833-b9f0-f0ab03749ffe","issue":"17","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"d127ff23-f9ea-4bcd-8226-8163acfab96f","keyword":"CdS","originalKeyword":"CdS"},{"id":"6c7897ee-57c7-442a-a959-f382b90cd4a1","keyword":"陶瓷<span style=\"color:red\">靶</span>材","originalKeyword":"陶瓷靶材"},{"id":"c189e081-3468-4415-bfaa-87c29b437fa2","keyword":"太阳能薄膜电池","originalKeyword":"太阳能薄膜电池"}],"language":"zh","publisherId":"gncl201517031","title":"硫化镉陶瓷<span style=\"color:red\">靶</span>材<span style=\"color:red\">的</span>制备<span style=\"color:red\">与</span>性能表征","volume":"","year":"2015"},{"abstractinfo":"针对9900型<span style=\"color:red\">靶</span>材<span style=\"color:red\">与</span>靶托<span style=\"color:red\">的</span>连接中存在<span style=\"color:red\">的</span>难题分析其原因, 对此采取了一些措施, 通过<span style=\"color:red\">靶</span>材大小, 焊料<span style=\"color:red\">的</span>改进和热处理等, 实现了Ni-Cr合金、铬、银<span style=\"color:red\">靶</span><span style=\"color:red\">与</span>铜底托<span style=\"color:red\">的</span>连接,生产出产品<span style=\"color:red\">的</span>批量使用证明, 焊接质量完全满足使用要求.","authors":[{"authorName":"韩雪","id":"32756964-5d9c-4ad1-85f1-36d95a530476","originalAuthorName":"韩雪"}],"doi":"10.3969/j.issn.0258-7076.2000.04.019","fpage":"317","id":"3f15e935-aa61-4d4b-8818-68c607e43230","issue":"4","journal":{"abbrevTitle":"XYJS","coverImgSrc":"journal/img/cover/XYJS.jpg","id":"67","issnPpub":"0258-7076","publisherId":"XYJS","title":"稀有金属"},"keywords":[{"id":"f2ff3280-a43b-4495-a046-58d330f40eb1","keyword":"<span style=\"color:red\">靶</span>材","originalKeyword":"靶材"},{"id":"c8120a9b-5ab9-4090-b1a4-1b25a59275b2","keyword":"靶托","originalKeyword":"靶托"},{"id":"defaacfd-8ba6-4fa1-a166-461c2c601c63","keyword":"连接","originalKeyword":"连接"},{"id":"c8950244-6af3-4be0-801f-5999255af654","keyword":"退火","originalKeyword":"退火"},{"id":"09db3b1e-15f0-470e-995f-508c340fe0ad","keyword":"脱焊","originalKeyword":"脱焊"}],"language":"zh","publisherId":"xyjs200004019","title":"9900型<span style=\"color:red\">靶</span>材<span style=\"color:red\">与</span>靶托<span style=\"color:red\">的</span>连接技术","volume":"24","year":"2000"},{"abstractinfo":"采用电子探针微分析术研究了机械复合和冶金复合两种界面状态<span style=\"color:red\">的</span>Nb-Ti/Cu复合超导线,以及Nb-Ti/Cu,Ti/Cu和Nb/Cu偶<span style=\"color:red\">的</span>扩散反应过程.结果表明,原始组件<span style=\"color:red\">的</span>界面状态对Nb-Ti/Cu间金属间化合物<span style=\"color:red\">的</span>生成有明显<span style=\"color:red\">的</span>影响.机械复合组件较冶金复合组件能承受更高<span style=\"color:red\">的</span>热处理温度而不致生成金属间化合物.Ti<span style=\"color:red\">与</span>Cu<span style=\"color:red\">之间</span>反应生成化合物<span style=\"color:red\">的</span>次序<span style=\"color:red\">与</span>形态及NbTi<span style=\"color:red\">与</span>Cu<span style=\"color:red\">之间</span>不同.Ti/Cu间生成化合物<span style=\"color:red\">的</span>厚度y<span style=\"color:red\">与</span>时间t关系遵循y~(1.5-t)<span style=\"color:red\">的</span>规律.","authors":[{"authorName":"徐乐英","id":"70f23851-0f3b-4749-bcfd-53d44e376a6f","originalAuthorName":"徐乐英"},{"authorName":"王文斌","id":"ccca181c-b0cb-4699-b9e1-6409f9ca6f72","originalAuthorName":"王文斌"},{"authorName":"庄育智","id":"fa5910c9-ef0e-49ac-a2f4-4492ab1acfb5","originalAuthorName":"庄育智"}],"categoryName":"|","doi":"","fpage":"335","id":"ff17f8cd-a0f2-4b07-b415-e4c2c5f8e4db","issue":"4","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"5c517f54-0030-4119-aaf1-26eafabe6c33","keyword":"Cu","originalKeyword":"Cu"},{"id":"b7e534a5-2dba-4ab2-9d7f-3334a7b31490","keyword":"NbTi alloy","originalKeyword":"NbTi alloy"},{"id":"f294cdf4-0003-44e3-8be0-12337fbf0571","keyword":"diffusion couple","originalKeyword":"diffusion couple"},{"id":"3896f972-f510-4a4c-b339-c200a90bae07","keyword":"superconductor","originalKeyword":"superconductor"},{"id":"e9393557-30a0-4f0b-8af2-eda82d5a8444","keyword":"diffusion reaction","originalKeyword":"diffusion reaction"}],"language":"zh","publisherId":"0412-1961_1988_4_21","title":"Cu<span style=\"color:red\">与</span>NbTi<span style=\"color:red\">之间</span>扩散反应<span style=\"color:red\">的</span>研究","volume":"24","year":"1988"},{"abstractinfo":"将冲击功分为温度敏感分量和非温度敏感分量,通过对断裂过程中能量<span style=\"color:red\">的</span>分析,认为冷脆性金属材料在下平台<span style=\"color:red\">的</span>断裂阻力主要决定于非温度敏感分量,在塑-脆过渡区,随着温度升高,温度敏感分量<span style=\"color:red\">的</span>作用越来越大.得到动态断裂韧度(KId)<span style=\"color:red\">与</span>冲击功(CVN)<span style=\"color:red\">之间</span><span style=\"color:red\">的</span>关系:K2Id=A+B(CVN),该式在上平台、塑-脆过渡区和下平台对KId<span style=\"color:red\">的</span>预测均与试验结果符合得比较满意.","authors":[{"authorName":"刘瑞堂","id":"e26249e3-9aa6-4d74-a967-db51cd4a3839","originalAuthorName":"刘瑞堂"},{"authorName":"王俊","id":"0c4658b6-5418-4eba-abe9-f63b5cd6d6bd","originalAuthorName":"王俊"}],"doi":"10.3969/j.issn.1001-4381.2003.z1.090","fpage":"271","id":"dfd40658-bcf8-4af1-8a26-4af6fe576812","issue":"z1","journal":{"abbrevTitle":"CLGC","coverImgSrc":"journal/img/cover/CLGC.jpg","id":"9","issnPpub":"1001-4381","publisherId":"CLGC","title":"材料工程"},"keywords":[{"id":"b5fa5b0e-accd-4972-88ed-70ec68f420cd","keyword":"动态断裂韧度","originalKeyword":"动态断裂韧度"},{"id":"c949380c-a984-4208-847c-56f80f9906ba","keyword":"示波冲击试验","originalKeyword":"示波冲击试验"},{"id":"ef5928c1-56e7-4e99-8fcd-6219ad3d33bf","keyword":"Charpy冲击功","originalKeyword":"Charpy冲击功"},{"id":"536b3ab9-6f0c-4cfa-8321-9a6df3602a76","keyword":"相关分析","originalKeyword":"相关分析"}],"language":"zh","publisherId":"clgc2003z1090","title":"动态断裂韧度<span style=\"color:red\">与</span>冲击功<span style=\"color:red\">之间</span>关系<span style=\"color:red\">的</span>探讨","volume":"","year":"2003"},{"abstractinfo":"散裂中子<span style=\"color:red\">靶</span>是加速器驱动洁净核能系统<span style=\"color:red\">的</span>一个重要环节. 相关<span style=\"color:red\">的</span>理论计算程序和蒙特-卡罗方法是研究该系统<span style=\"color:red\">的</span>散裂<span style=\"color:red\">靶</span>物理<span style=\"color:red\">的</span>一个重要手段. 对相关程序进行了比对和介绍, 并对SHIELD程序系统在中国<span style=\"color:red\">的</span>发展和在散裂<span style=\"color:red\">靶</span>物理上<span style=\"color:red\">的</span>应用作了介绍. ","authors":[{"authorName":"樊胜","id":"378ff75e-f424-4a87-a9c0-780220cfee5a","originalAuthorName":"樊胜"},{"authorName":"于洪伟","id":"b408eadd-3875-4d93-b6f1-3d5466c5a3aa","originalAuthorName":"于洪伟"},{"authorName":"申庆彪","id":"3d4d8df1-f825-4dda-ab64-b61acf5afc59","originalAuthorName":"申庆彪"},{"authorName":"赵志祥","id":"afc00b07-fa3c-4b47-8831-3cb5b069bc71","originalAuthorName":"赵志祥"}],"doi":"10.3969/j.issn.1007-4627.2002.04.005","fpage":"390","id":"adae6e98-3d4a-47db-864a-01ef1d8efda4","issue":"4","journal":{"abbrevTitle":"YZHWLPL","coverImgSrc":"journal/img/cover/YZHWLPL.jpg","id":"78","issnPpub":"1007-4627","publisherId":"YZHWLPL","title":"原子核物理评论   "},"keywords":[{"id":"85a7b487-7876-4b1e-b4ce-3803d5b871be","keyword":"散裂中子<span style=\"color:red\">靶</span>","originalKeyword":"散裂中子靶"},{"id":"e2e0dcfb-1420-465a-916b-243f05b4bf42","keyword":"计算程序","originalKeyword":"计算程序"},{"id":"422bb266-22df-46c3-bd85-5f47d5fbf07e","keyword":"加速器驱动系统","originalKeyword":"加速器驱动系统"}],"language":"zh","publisherId":"yzhwlpl200204005","title":"<span style=\"color:red\">与</span>散裂中子<span style=\"color:red\">靶</span>物理相关<span style=\"color:red\">的</span>理论计算程序探讨II 厚<span style=\"color:red\">靶</span>计算","volume":"19","year":"2002"},{"abstractinfo":"本文在文献研究<span style=\"color:red\">的</span>基础上,设计了一种简单易行<span style=\"color:red\">的</span>试验装置,通过直剪试验测定复合纤维布<span style=\"color:red\">与</span>混凝土<span style=\"color:red\">之间</span><span style=\"color:red\">的</span>粘结强度,得出各测点离端部<span style=\"color:red\">距离</span>-应变关系曲线,进而绘出复合纤维布中沿粘结方向<span style=\"color:red\">的</span>粘结应力分布,以确定有效粘结长度.所得初步结论为梁抗弯、抗剪加固<span style=\"color:red\">的</span>粘结提供设计参数.","authors":[{"authorName":"肖建庄","id":"52068f0c-07ad-4c9a-ab41-c86f5a3c4053","originalAuthorName":"肖建庄"},{"authorName":"李杰","id":"06b8ade3-b10b-4746-a11b-03aafc847eeb","originalAuthorName":"李杰"},{"authorName":"魏锦涛","id":"f008a4cd-c36c-43a5-8373-0fa8b3b95f1a","originalAuthorName":"魏锦涛"}],"doi":"10.3969/j.issn.1003-0999.2002.03.001","fpage":"3","id":"079d58db-11a3-44ec-9b9e-e2d486d3ee45","issue":"3","journal":{"abbrevTitle":"BLGFHCL","coverImgSrc":"journal/img/cover/BLGFHCL.jpg","id":"6","issnPpub":"1003-0999","publisherId":"BLGFHCL","title":"玻璃钢/复合材料"},"keywords":[{"id":"cf70d3d8-0b14-47e2-ab18-1e2c6d14825c","keyword":"复合纤维布","originalKeyword":"复合纤维布"},{"id":"0754285c-f9d3-453d-ab20-2df5bc75b481","keyword":"混凝土","originalKeyword":"混凝土"},{"id":"507fd7a5-cc90-4871-8b94-14007d7ec9b4","keyword":"粘结力","originalKeyword":"粘结力"},{"id":"85a90083-af76-4db3-bc8d-29c75ed5d1de","keyword":"试验方法","originalKeyword":"试验方法"}],"language":"zh","publisherId":"blgfhcl200203001","title":"纤维布<span style=\"color:red\">与</span>混凝土<span style=\"color:red\">之间</span>粘结力<span style=\"color:red\">的</span>试验方法研究","volume":"","year":"2002"}],"totalpage":21676,"totalrecord":216759}