{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"采用硼硅酸盐玻璃与氧化铝复合烧结制备了硼硅酸盐玻璃/Al2O3系低温共烧陶瓷基板材料,研究了玻璃含量以及玻璃中碱金属离子的含量对介电性能的影响.结果表明,该体系复合材料介电常数随碱金属离子的增加有所增大,复合材料介电常数符合李赫德涅凯对数法则,并随复合材料玻璃含量的增加而减小;复合材料介质损耗随碱金属离子的增加而显著增大.","authors":[{"authorName":"<span style=\"color:red\">陈</span><span style=\"color:red\">兴</span><span style=\"color:red\">宇</span>","id":"fa685afa-b215-4321-abbf-f18856616f42","originalAuthorName":"陈兴宇"},{"authorName":"张为军","id":"c8798c63-bac7-4d34-9157-6cc495c5003d","originalAuthorName":"张为军"},{"authorName":"堵永国","id":"30a6d099-e6b5-4ac2-a327-6947d9df1d1e","originalAuthorName":"堵永国"},{"authorName":"胡君遂","id":"6465f5cd-fafe-4429-b7ff-cb63455dcd18","originalAuthorName":"胡君遂"},{"authorName":"郑晓慧","id":"2c9f2ac2-7348-4d82-bbaf-8cbe45d77e66","originalAuthorName":"郑晓慧"},{"authorName":"芦玉峰","id":"6aeff642-b49e-4ba7-ba06-d84f84c24e69","originalAuthorName":"芦玉峰"}],"doi":"","fpage":"1146","id":"6052dd25-4c92-4fb2-b398-fa517efebf05","issue":"6","journal":{"abbrevTitle":"GSYTB","coverImgSrc":"journal/img/cover/GSYTB.jpg","id":"36","issnPpub":"1001-1625","publisherId":"GSYTB","title":"硅酸盐通报   "},"keywords":[{"id":"a10cffd2-ac8c-4027-9c52-9bee5b73f9c6","keyword":"低温共烧陶瓷","originalKeyword":"低温共烧陶瓷"},{"id":"21558980-cc8b-4505-95da-ac279704cdd0","keyword":"硼硅酸盐玻璃/Al2O3","originalKeyword":"硼硅酸盐玻璃/Al2O3"},{"id":"2d464061-d227-47e1-917f-8a72fac0da5f","keyword":"介电常数","originalKeyword":"介电常数"},{"id":"f6909595-097f-4445-ac1f-c8814b707682","keyword":"介质损耗","originalKeyword":"介质损耗"}],"language":"zh","publisherId":"gsytb200806012","title":"硼硅酸盐玻璃/Al2O3低温共烧陶瓷介电性能研究","volume":"27","year":"2008"},{"abstractinfo":"掺杂不仅改变石墨块体材料的成分,还可以改变其微观形貌和微观结构,进而影响材料的力学性能、导热性能、导电性能和抗氧化性能.在总结石墨掺杂改性的方法和石墨掺杂改性原理的基础上,综述了目前国内外掺杂石墨材料的研究现状.","authors":[{"authorName":"华叶","id":"73ad13da-cef9-4427-ad64-12c60c0900f5","originalAuthorName":"华叶"},{"authorName":"万红","id":"b6d5a9e4-6ef6-42e7-91de-e815d0bab8bd","originalAuthorName":"万红"},{"authorName":"<span style=\"color:red\">陈</span><span style=\"color:red\">兴</span><span style=\"color:red\">宇</span>","id":"01513176-276d-4bae-962f-d04fce152dc2","originalAuthorName":"陈兴宇"}],"doi":"10.11896/j.issn.1005-023X.2015.05.005","fpage":"25","id":"4b955f0a-0728-4af8-ad77-4de157dd33b1","issue":"5","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"8c7ca1ce-6acc-4ce1-8ccc-d5b0fafe3f63","keyword":"掺杂改性","originalKeyword":"掺杂改性"},{"id":"ba3c9e85-aa98-4693-a5a2-75fc14052371","keyword":"液相浸渍","originalKeyword":"液相浸渍"},{"id":"f372e85f-d4f0-4146-8e81-9aba75ab8a01","keyword":"气相沉积","originalKeyword":"气相沉积"},{"id":"63521094-5269-4cda-9ac0-da5341fb6d00","keyword":"微观形貌","originalKeyword":"微观形貌"},{"id":"baa01d25-ad4f-4aeb-8173-2f043e178e3a","keyword":"微观结构","originalKeyword":"微观结构"}],"language":"zh","publisherId":"cldb201505005","title":"石墨材料的掺杂改性及其研究现状","volume":"29","year":"2015"},{"abstractinfo":"将具有负<span style=\"color:red\">宇</span>称的 fp 空间扩大到包含1g9/2 轨道, 采用修正的表面相互作用(MSDI), 对64Ge, 66Ge, 68Ge, 70Se, 72Se, 74Se, 76Kr 和 78Kr等偶偶核作了形变Hartree-Fock计算, 得到了基态和一些激发态的解. 同时, 还用近似角动量投影形变Hartree-Fock(PDHF)方法对偶偶核64Ge, 74Se和奇A核79Kr进行了能谱计算, 得到其正、负<span style=\"color:red\">宇</span>称带的解, 计算结果与实验谱基本一致.","authors":[{"authorName":"徐延冰","id":"b1aeaa3f-d49e-4faa-b5c2-14d575021e7a","originalAuthorName":"徐延冰"}],"doi":"10.3969/j.issn.1007-4627.2004.01.002","fpage":"6","id":"3d804ba2-a11b-4d98-b76a-e37dcc73a053","issue":"1","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":"3c3761e3-ccf3-4809-86d9-25135f7d42e0","keyword":"形变Hartree-Fock态","originalKeyword":"形变Hartree-Fock态"},{"id":"1432f8a8-2714-44ab-8011-bf4d80e7029c","keyword":"角动量投影","originalKeyword":"角动量投影"},{"id":"ed3d33ae-e94a-4a28-ab9a-4dc4a49250a9","keyword":"单粒子能谱","originalKeyword":"单粒子能谱"},{"id":"aebc8a5b-b795-4038-9aaf-a485915d7835","keyword":"反常<span style=\"color:red\">宇</span>称态","originalKeyword":"反常宇称态"}],"language":"zh","publisherId":"yzhwlpl200401002","title":"原子核的反常<span style=\"color:red\">宇</span>称能谱研究","volume":"21","year":"2004"},{"abstractinfo":"将具有正<span style=\"color:red\">宇</span>称的gds组态空间扩大到包含具有负<span style=\"color:red\">宇</span>称的1h11/2轨道, 采用修正的表面δ相互作用(MSDI)对101Pd和101Ru两个奇A 核进行了形变HF计算, 得到了基态和一些激发态的解. 同时, 还用近似角动量投影形变Hartree-Fock(PDHF)方法对101Pd和101Ru进行了能谱计算, 得到其正、负<span style=\"color:red\">宇</span>称带的解, 计算结果与实验谱基本一致.","authors":[{"authorName":"徐延冰","id":"1b3ba6c1-1a0a-40d8-8d0e-634c29ad7ad3","originalAuthorName":"徐延冰"}],"doi":"10.3969/j.issn.1007-4627.2003.03.003","fpage":"182","id":"8ca98726-f9ca-4b95-a219-e8c108fbc41b","issue":"3","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":"ea28bceb-8a87-4ceb-a831-8675db84565c","keyword":"角动量投影","originalKeyword":"角动量投影"},{"id":"41e3bba1-73a3-43b6-8267-e18bda970894","keyword":"单粒子能谱","originalKeyword":"单粒子能谱"},{"id":"c5c9cb2d-cbfb-46ab-8403-666a47a2276d","keyword":"负<span style=\"color:red\">宇</span>称带","originalKeyword":"负宇称带"}],"language":"zh","publisherId":"yzhwlpl200303003","title":"奇A核101Pd和101Ru的负<span style=\"color:red\">宇</span>称带能谱研究","volume":"20","year":"2003"},{"abstractinfo":"以能量为1.5 MeV/u，剂量分别为500，750，1000，1250，1500 Gy的电子束对1，2，4，6，8年等5种年份浓香型白酒进行辐照处理；扫描各酒样200～400 nm波段的紫外光谱，根据紫外光谱图的差异，计算了280～300 nm波段的光谱曲线相似度，分析光谱曲线变化规律。结果表明，对于前4种白酒，对照样与辐照样光谱曲线相似度值越小，催<span style=\"color:red\">陈</span>效果越好；白酒存放时间越久，酒体风格转向老熟所需剂量越小，越容易达到最佳催<span style=\"color:red\">陈</span>效果；对于8年白酒，辐照剂量超过750 Gy后，白酒体系动态平衡被打破，各单体物质增加，出现返生现象。因此，电子束辐照技术对低年份浓香型白酒催<span style=\"color:red\">陈</span>效果显著，是一种先进、高效的催<span style=\"color:red\">陈</span>方法。","authors":[{"authorName":"张苗苗","id":"16f2bee9-e276-4f55-95b1-9e627a4ac276","originalAuthorName":"张苗苗"},{"authorName":"陆栋","id":"6bd2c6ff-fa0f-4deb-9553-bfa0e40d3ab7","originalAuthorName":"陆栋"},{"authorName":"曹国珍","id":"ad44f083-8f23-4d8d-a41c-b6321e181155","originalAuthorName":"曹国珍"},{"authorName":"刘敬","id":"980de600-54b3-4c10-b2b1-7d36c88bd704","originalAuthorName":"刘敬"},{"authorName":"金文杰","id":"9d97782b-4400-438f-aa1a-efaa2ae74455","originalAuthorName":"金文杰"},{"authorName":"王菊芳","id":"7a171c96-4419-441c-8118-cabb35cc1b2c","originalAuthorName":"王菊芳"},{"authorName":"李文建","id":"db0225a5-b939-440c-a47d-2daa37f339b7","originalAuthorName":"李文建"}],"doi":"10.11804/NuclPhysRev.31.02.218","fpage":"218","id":"be399f10-d5ab-444a-9853-693337e4845a","issue":"2","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":"d27824cd-9a7d-40d6-ade5-08e57f3651e9","keyword":"白酒","originalKeyword":"白酒"},{"id":"a87d8a5f-52c5-438d-9818-ac05aa030ecd","keyword":"电子束","originalKeyword":"电子束"},{"id":"59b3d998-0774-4358-b00a-6ad942d1d4f2","keyword":"紫外可见光谱","originalKeyword":"紫外可见光谱"},{"id":"7662c117-7566-4173-b784-d5cf69060062","keyword":"光谱曲线相似度","originalKeyword":"光谱曲线相似度"},{"id":"ef90b8b5-c334-453a-8346-0f1341f1e34b","keyword":"催<span style=\"color:red\">陈</span>效果","originalKeyword":"催陈效果"}],"language":"zh","publisherId":"yzhwlpl201402017","title":"电子束辐照浓香型白酒催<span style=\"color:red\">陈</span>效果的研究","volume":"","year":"2014"},{"abstractinfo":"根据炮钢材料的拉伸－压缩特性，通过模拟实验，建立了以鲍<span style=\"color:red\">兴</span>格效应系数为函数计算自紧身管壁内任意一点残余应力的理论模型。与以往不同的是利用炮钢材料的拉伸－压缩试样，通过拉伸－压缩实验用最小二乘法拟合出鲍<span style=\"color:red\">兴</span>格效应系数与壁内最大拉伸变形量的关系。在计算自紧身管残余应力时，鲍<span style=\"color:red\">兴</span>格效应系数不再被视为常量而被视为变量，因此，这就克服了以往鲍<span style=\"color:red\">兴</span>格效应系数取平均值所带来的误差。本文采用修正的Mises屈服准则以及形变理论，按广义平面应变问题，建立了强化材料的应力应变模型，导出了具有应变硬化，鲍<span style=\"color:red\">兴</span>格效应系数被视为变量的强化材料液压自紧圆筒的残余应力公式。实验也表明：用鲍<span style=\"color:red\">兴</span>格系数为变量的理论模型进行炮钢材料自紧身管的残余应力计算更合理，更能反映自紧火炮身管的实际状态。","authors":[{"authorName":"马绍华","id":"6b60149d-1be5-4dc9-ba41-daa1cab32a1b","originalAuthorName":"马绍华"},{"authorName":"任安峰","id":"fff1b931-79a6-4385-b39f-88ab22f7c490","originalAuthorName":"任安峰"},{"authorName":"李贵才","id":"7794ef88-0d75-4e0a-9484-35aed4f5fbe0","originalAuthorName":"李贵才"},{"authorName":"黄建文","id":"41dd7822-9cb2-4e95-8926-070f26beb5d1","originalAuthorName":"黄建文"},{"authorName":"董方","id":"ee8e5208-6228-469e-92b6-002609b053a4","originalAuthorName":"董方"}],"doi":"10.3969/j.issn.1004-244X.2001.01.012","fpage":"44","id":"caffd856-9a00-44e5-b71a-bfa29086d635","issue":"1","journal":{"abbrevTitle":"BQCLKXYGC","coverImgSrc":"journal/img/cover/BQCLKXYGC.jpg","id":"4","issnPpub":"1004-244X","publisherId":"BQCLKXYGC","title":"兵器材料科学与工程   "},"keywords":[{"id":"7241be77-aead-4517-bd9d-b95473011f09","keyword":"鲍<span style=\"color:red\">兴</span>格效应","originalKeyword":"鲍兴格效应"},{"id":"187c9de5-19d9-4856-96cd-50c0547f908b","keyword":"自紧身管","originalKeyword":"自紧身管"},{"id":"b55e9314-0791-49b9-be8b-c1ec79036d61","keyword":"残余应力","originalKeyword":"残余应力"}],"language":"zh","publisherId":"bqclkxygc200101012","title":"鲍<span style=\"color:red\">兴</span>格效应对自紧身管残余应力影响规律的研究","volume":"24","year":"2001"},{"abstractinfo":"通过光片鉴定和电子探针分析,总结了内蒙古赤峰<span style=\"color:red\">陈</span>家杖子金矿床的矿石矿物组成,结构构造,划分了成矿期次.研究表明:矿床中矿石成分较复杂,硫化物种类多,有少量硫盐矿物出现;富硫贫砷毒砂、贫砷富硫黄铁矿、贫锌富铁的闪锌矿(与标准分子式相比),含杂质多的银锑黝铜矿和方铅矿与金关系密切;多金属硫化物阶段是该矿床的主要成矿阶段,其中第二世代富硫贫砷毒砂是<span style=\"color:red\">陈</span>家杖子金矿的最主要载金矿物,其次是方铅矿.结合流体包裹体测试和研究,确定该矿床为受大型角砾岩筒构造控制的低硫化型浅成低温热液矿床,该矿床深部有很大的找矿潜力.","authors":[{"authorName":"霍亮","id":"aa8459a3-b8df-471f-beb6-c0820f947fb7","originalAuthorName":"霍亮"},{"authorName":"李碧乐","id":"0542a65f-639d-436f-9395-33a31da28fa5","originalAuthorName":"李碧乐"},{"authorName":"黄勇","id":"c3eb9700-f7a0-4640-951f-31133483900c","originalAuthorName":"黄勇"},{"authorName":"王力","id":"74c22902-9e7c-40f8-8cad-6d663cf193da","originalAuthorName":"王力"}],"doi":"10.3969/j.issn.1001-1277.2007.10.002","fpage":"4","id":"d9d6227a-88ea-4727-89c6-a72289a7a8f9","issue":"10","journal":{"abbrevTitle":"HJ","coverImgSrc":"journal/img/cover/HJ.jpg","id":"44","issnPpub":"1001-1277","publisherId":"HJ","title":"黄金"},"keywords":[{"id":"342763a1-a09a-4924-a3cd-d93fd15d2580","keyword":"矿石矿物特征","originalKeyword":"矿石矿物特征"},{"id":"5ed5d2c9-7efa-4ac6-91b8-a288a651641c","keyword":"矿床成因","originalKeyword":"矿床成因"},{"id":"196f3b92-1f65-4e1d-a829-9ab98bb8b116","keyword":"<span style=\"color:red\">陈</span>家杖子金矿床","originalKeyword":"陈家杖子金矿床"}],"language":"zh","publisherId":"huangj200710002","title":"内蒙古赤峰<span style=\"color:red\">陈</span>家杖子金矿床矿物学特征及成因","volume":"28","year":"2007"},{"abstractinfo":"北<span style=\"color:red\">兴</span>特钢\"四位一体\"短流程生产线2002年11月热试车以来,为了早日实现达产、达效,进行了连铸中间罐快换试验.本文从工艺准备,操作过程控制等方面,介绍中间罐快换的生产经验.","authors":[{"authorName":"刘乐东","id":"c91141c0-5cd6-4612-8829-bf7aecc483a0","originalAuthorName":"刘乐东"},{"authorName":"李英武","id":"2fc6c56e-ae8a-416d-b063-c75ae839b83f","originalAuthorName":"李英武"},{"authorName":"李彦军","id":"74244cf9-0d51-42cf-964c-119b6ad8453e","originalAuthorName":"李彦军"}],"doi":"10.3969/j.issn.1005-4006.2005.05.005","fpage":"14","id":"e673b9f3-7bfc-4d39-bcab-a99a4b5ab983","issue":"5","journal":{"abbrevTitle":"LZ","coverImgSrc":"journal/img/cover/LZ.jpg","id":"52","issnPpub":"1005-4006","publisherId":"LZ","title":"连铸"},"keywords":[{"id":"a7b10bd0-9a13-4bce-9274-2bd5debbb1bc","keyword":"","originalKeyword":""}],"language":"zh","publisherId":"lz200505005","title":"北<span style=\"color:red\">兴</span>特钢连铸中间罐快换的生产实践","volume":"","year":"2005"},{"abstractinfo":"分别利用单胶子交换和单π交换夸克模型计算了核子负<span style=\"color:red\">宇</span>称激发态的电磁跃迁振幅, 讨论了两个模型所给出的不同的组态混合角.结果表明,单胶子交换模型所给出的重子波函数比单π交换夸克模型的波函数更为合理.","authors":[{"authorName":"董<span style=\"color:red\">宇</span>兵","id":"83ccf7c3-5aa4-4ac7-9522-e880eef67f74","originalAuthorName":"董宇兵"},{"authorName":"何军","id":"a80d2e96-ebcc-41e0-a019-3bf8b76e9153","originalAuthorName":"何军"}],"doi":"10.3969/j.issn.1007-4627.2004.02.023","fpage":"157","id":"e1fe2c51-b3cd-4c86-89e8-4ee665f93740","issue":"2","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":"a63ab8b9-3465-4019-92af-021ca69cedbc","keyword":"组份夸克模型","originalKeyword":"组份夸克模型"},{"id":"a60932b0-1801-4191-91e0-fd4a7483cb8f","keyword":"组态混合","originalKeyword":"组态混合"},{"id":"78c8f132-1bf4-487f-9660-41c2958cb36f","keyword":"跃迁振幅","originalKeyword":"跃迁振幅"}],"language":"zh","publisherId":"yzhwlpl200402023","title":"单胶子交换和单π交换夸克模型中核子负<span style=\"color:red\">宇</span>称共振态的电磁跃迁振幅","volume":"21","year":"2004"},{"abstractinfo":"针对田<span style=\"color:red\">兴</span>铁矿1＃主井井壁突水情况及井壁裂隙破碎带的结构特点，介绍了在出水点埋设3根导水管将井壁涌水引入工作面水窝，再浇筑混凝土井壁形成支撑结构防止围岩失稳、裂隙扩展，最后待浇筑混凝土养护后对其壁后注浆封水的突水治理方案。其中，壁后注浆采用上行式注浆，由下而上逐步推进注浆封水，注浆孔分3层上下菱形交错布置。经过井壁突水综合治理方案的实施，田<span style=\"color:red\">兴</span>铁矿1＃主井井壁裂隙破碎带涌水从最初的64 m3／h降到近20 m3／h，对井壁涌水起到了封堵作用，有效保障了后续井筒下掘施工的安全。","authors":[{"authorName":"翟会超","id":"c2216963-8e99-40a3-990a-42d695d27d27","originalAuthorName":"翟会超"},{"authorName":"南世卿","id":"a4f5df41-1fb1-4bfd-9699-b2db8f53510c","originalAuthorName":"南世卿"},{"authorName":"胡巍巍","id":"cc485eb9-739d-4ced-b4aa-9e4447adaa2f","originalAuthorName":"胡巍巍"}],"doi":"10.11792/hj20150110","fpage":"40","id":"2a66741a-c833-4cc8-b3e5-c69bc80e2bd6","issue":"1","journal":{"abbrevTitle":"HJ","coverImgSrc":"journal/img/cover/HJ.jpg","id":"44","issnPpub":"1001-1277","publisherId":"HJ","title":"黄金"},"keywords":[{"id":"9f52f223-bb5c-4994-ad00-534efca33f40","keyword":"竖井","originalKeyword":"竖井"},{"id":"9c307991-cead-489b-89dd-45dca92e5b8b","keyword":"壁后注浆","originalKeyword":"壁后注浆"},{"id":"a60413ca-55c6-4719-95b3-02371724057b","keyword":"导水","originalKeyword":"导水"},{"id":"7fc8410d-06ba-47d9-8309-48540836705c","keyword":"井壁支护","originalKeyword":"井壁支护"},{"id":"64e4e238-74df-4901-8f05-78a41a94d22d","keyword":"稳定性","originalKeyword":"稳定性"}],"language":"zh","publisherId":"huangj201501013","title":"田<span style=\"color:red\">兴</span>铁矿1主井施工突水治理工程实践","volume":"","year":"2015"}],"totalpage":11,"totalrecord":106}