{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"通过对中国黄金集团公司等四大黄金集团资源占有情况的总结分析,阐述了中国黄金矿业企业进一步开展资源整合、资源并购、生产探矿及风险探矿等资源占有工作,对矿山延长服务年限、企业结构调整及加速国际化进程,从而实现中国黄金矿业企业在“十二五”及更远时期内可持续发展的重要意义.","authors":[{"authorName":"<span style=\"color:red\">傅</span><span style=\"color:red\">渊</span><span style=\"color:red\">慧</span>","id":"ce7ea896-ee27-4ea0-a851-2838d702ad2e","originalAuthorName":"傅渊慧"},{"authorName":"杨志刚","id":"9626635a-6864-4402-9354-02847ed00868","originalAuthorName":"杨志刚"},{"authorName":"高世贤","id":"17a6507f-e5ac-42ef-ac58-63a884b50ae2","originalAuthorName":"高世贤"},{"authorName":"杨春福","id":"47a6ea9e-0734-4e41-8ff3-622aa8b4c003","originalAuthorName":"杨春福"},{"authorName":"黄绍锋","id":"b315a8da-60bc-443d-af72-e0427adb91d5","originalAuthorName":"黄绍锋"}],"doi":"10.3969/j.issn.1001-1277.2011.09.001","fpage":"1","id":"77bb5ded-891d-4362-9c0d-3e07e0eb6fa7","issue":"9","journal":{"abbrevTitle":"HJ","coverImgSrc":"journal/img/cover/HJ.jpg","id":"44","issnPpub":"1001-1277","publisherId":"HJ","title":"黄金"},"keywords":[{"id":"7ea914af-22fb-4477-944a-bc38ac774b8c","keyword":"黄金矿业","originalKeyword":"黄金矿业"},{"id":"11f1f21e-73ca-4beb-abfd-21df13f0b838","keyword":"资源占有","originalKeyword":"资源占有"},{"id":"c47d7369-f405-4444-8dd7-6ee246d20d3b","keyword":"结构调整","originalKeyword":"结构调整"},{"id":"01394b0a-9020-419e-85bd-8bfc185db2fe","keyword":"国际化","originalKeyword":"国际化"},{"id":"ba3fca7c-abe7-4fde-9e09-972580af8de4","keyword":"可持续发展","originalKeyword":"可持续发展"}],"language":"zh","publisherId":"huangj201109001","title":"论资源占有对中国黄金矿业企业可持续发展的意义","volume":"32","year":"2011"},{"abstractinfo":"利用Richarda-Wolf矢量衍射积分公式,获得矢量偏振贝塞耳-高斯光束经具有初级<span style=\"color:red\">慧</span>差的高数值孔径系统聚焦后的三维光场复振幅函数,模拟了不同<span style=\"color:red\">慧</span>差系数下聚焦光场的纵向分布,以及焦平面和光轴上的光强.研究表明,初级<span style=\"color:red\">慧</span>差的存在导致矢量偏振贝塞耳-高斯光束的会聚光场发生偏移和变形,焦平面光强的分布和光轴上的光强峰值都受初级<span style=\"color:red\">慧</span>差和入射光偏振态的共同影响,偏振态和初级<span style=\"color:red\">慧</span>差不影响聚焦光场在光轴上的对称分布.","authors":[{"authorName":"赵肇雄","id":"351f79cc-aff5-4f3a-9fbc-07bc2b931a61","originalAuthorName":"赵肇雄"},{"authorName":"刘勇","id":"17bc2344-39e3-41ae-a78a-49d6e0645aeb","originalAuthorName":"刘勇"}],"doi":"10.3969/j.issn.1007-5461.2009.06.001","fpage":"641","id":"eb449bfc-7d52-4398-a1e8-0b4dc3bd13fc","issue":"6","journal":{"abbrevTitle":"LZDZXB","coverImgSrc":"journal/img/cover/LZDZXB.jpg","id":"53","issnPpub":"1007-5461","publisherId":"LZDZXB","title":"量子电子学报   "},"keywords":[{"id":"62d210fb-f736-4137-8c1a-62981757c789","keyword":"物理光学","originalKeyword":"物理光学"},{"id":"49c0f2d4-b533-44d6-b572-42938dd4503c","keyword":"贝塞耳-高斯光束","originalKeyword":"贝塞耳-高斯光束"},{"id":"a254e378-38df-4f80-92a9-d6853b7b09e9","keyword":"Richards-Wolf矢量衍射积分","originalKeyword":"Richards-Wolf矢量衍射积分"},{"id":"05fea4e3-fbf6-401f-a1ca-83848bac5ffd","keyword":"径向偏振","originalKeyword":"径向偏振"},{"id":"957bc8e8-42db-4b4e-bfb3-439486541c6f","keyword":"方位角偏振","originalKeyword":"方位角偏振"},{"id":"05e85e96-245d-4961-af12-e34907e1041a","keyword":"<span style=\"color:red\">慧</span>差","originalKeyword":"慧差"}],"language":"zh","publisherId":"lzdzxb200906001","title":"<span style=\"color:red\">慧</span>差对矢量偏振贝塞耳-高斯光束聚焦场的影响","volume":"26","year":"2009"},{"abstractinfo":"由于受激布里渊散射(SBS)介质大多为液体和气体,当提高重复运转频率或延长泵浦脉冲的持续时间时,其中的热积累和热驰豫将严重影响甚至破坏SBS的形成及其共轭品质.为改善SBS在高重复频率下的工作性能,实验考察了具有SBS相位共轭镜的MOPA(Master-oscillator-power-amplifier)系统中泵浦光发散度对布里<span style=\"color:red\">渊</span>池重复运转特性的影响.结果表明:降低泵浦光发散度有利于提高布里<span style=\"color:red\">渊</span>池的重复运转频率及改善SBS的时空特性,但会增加SBS阈值,减小布里<span style=\"color:red\">渊</span>池工作的泵浦能量范围,同时,保真度略有下降.","authors":[{"authorName":"刘安玲","id":"337628fd-ec26-4d4a-99de-054084346b20","originalAuthorName":"刘安玲"},{"authorName":"张为俊","id":"254d4794-6e12-49e2-a367-3f7c5a05082d","originalAuthorName":"张为俊"},{"authorName":"高晓明","id":"c735e424-e5db-4781-a604-0c1714e2bf64","originalAuthorName":"高晓明"}],"doi":"10.3969/j.issn.1007-5461.2008.02.018","fpage":"221","id":"88fc6ab6-dd45-4c00-aa95-6aeb3d9d0715","issue":"2","journal":{"abbrevTitle":"LZDZXB","coverImgSrc":"journal/img/cover/LZDZXB.jpg","id":"53","issnPpub":"1007-5461","publisherId":"LZDZXB","title":"量子电子学报   "},"keywords":[{"id":"d6860259-cc03-493e-aaa8-ab78bdfcf8ed","keyword":"非线性光学","originalKeyword":"非线性光学"},{"id":"f1490f60-e9e3-4f6e-a71c-b8aeec2d1280","keyword":"受激布里渊散射","originalKeyword":"受激布里渊散射"},{"id":"e23b8e2c-e37e-4d6f-976a-386c1430bd9e","keyword":"发散度","originalKeyword":"发散度"},{"id":"23ce4e92-16ba-4634-a35f-e4ec7c93c689","keyword":"重复频率","originalKeyword":"重复频率"}],"language":"zh","publisherId":"lzdzxb200802018","title":"泵浦光发散度对布里<span style=\"color:red\">渊</span>池重复运转特性的影响","volume":"25","year":"2008"},{"abstractinfo":"利用二次量子化方法研究了由相同面心立方结构(100)材料构成的铁磁性双层薄膜,重点讨论了铁磁性界面交换作用(JABB>0)和反铁磁性界面交换作用(JAB<0)对体系二维布里<span style=\"color:red\">渊</span>区能带结构的影响.结果表明,当界面交换作用大于体交换作用时,在体模上方出现光学型界面模;当界面交换作用小于体交换作用时,在体模下方出现声学型界面模.特别的是,当铁磁性界面交换作用大小在零与体交换作用之间时,在面心立方结构中同样能出现声学型界面模,这与简立方结构有明显区别.并且讨论了不同界面交换作用时宇称对界面模的影响.","authors":[{"authorName":"史晓霞","id":"60b813a5-f1f6-465d-b35b-94a770bc9007","originalAuthorName":"史晓霞"},{"authorName":"云国宏","id":"38f9d486-e30e-4134-b5b2-85bfcc7dd330","originalAuthorName":"云国宏"},{"authorName":"周文平","id":"da132d85-4f02-47d0-b737-3b1b48dd7f45","originalAuthorName":"周文平"}],"doi":"","fpage":"458","id":"169d9650-a2b2-4aa9-ba5f-d3567ef6c59a","issue":"6","journal":{"abbrevTitle":"DWWLXB","coverImgSrc":"journal/img/cover/DWWLXB.jpg","id":"19","issnPpub":"1000-3258","publisherId":"DWWLXB","title":"低温物理学报   "},"keywords":[{"id":"c9dacaab-31dd-4df9-9e8b-ec34c6943643","keyword":"铁磁性双层薄膜","originalKeyword":"铁磁性双层薄膜"},{"id":"5ed66aed-85d1-4226-acc5-4292fec8f658","keyword":"面心立方","originalKeyword":"面心立方"},{"id":"226e6488-2357-4096-aaf2-51bd18b1080f","keyword":"界面交换作用","originalKeyword":"界面交换作用"},{"id":"e3e182f2-7011-49df-a31c-734e95708452","keyword":"界面模","originalKeyword":"界面模"},{"id":"6c24e138-4a8f-4752-a60e-671ca674d241","keyword":"体模","originalKeyword":"体模"}],"language":"zh","publisherId":"dwwlxb201006012","title":"面心立方双层铁磁薄膜中的二维布里<span style=\"color:red\">渊</span>区能带结构","volume":"32","year":"2010"},{"abstractinfo":"提出了自<span style=\"color:red\">傅</span>里叶孤子概念.对自<span style=\"color:red\">傅</span>里叶孤子信号及自<span style=\"color:red\">傅</span>里叶高斯信号在光纤中的演变和传输进行了数值模拟和时频分析.结果表明,输入自<span style=\"color:red\">傅</span>里叶高斯信号,将演变成一类非自<span style=\"color:red\">傅</span>里叶孤子;三阶色散效应会影响由自<span style=\"color:red\">傅</span>里叶高斯信号所演变的孤子的震荡传输幅度,且引起孤子时域延迟、频谱不对称.","authors":[{"authorName":"殷德京","id":"ba1b2ca6-95d9-49c1-ba20-2318cc6e727a","originalAuthorName":"殷德京"}],"doi":"10.3969/j.issn.1007-5461.2009.04.021","fpage":"499","id":"dc0fd06c-9b69-42e8-ba36-242b96a2fe20","issue":"4","journal":{"abbrevTitle":"LZDZXB","coverImgSrc":"journal/img/cover/LZDZXB.jpg","id":"53","issnPpub":"1007-5461","publisherId":"LZDZXB","title":"量子电子学报   "},"keywords":[{"id":"a13c83eb-0099-46fe-ad71-a2123245081d","keyword":"纤维与波导光学","originalKeyword":"纤维与波导光学"},{"id":"c0603d72-8dfc-44bc-8cde-d56d8e16ba04","keyword":"自<span style=\"color:red\">傅</span>里叶信号","originalKeyword":"自傅里叶信号"},{"id":"b32eae57-cbc7-4c94-a1e9-8667e90d3d45","keyword":"分步傅里叶变换方法","originalKeyword":"分步傅里叶变换方法"},{"id":"e754e6fc-616a-4af4-aac5-c2ba3099dad8","keyword":"孤子分裂","originalKeyword":"孤子分裂"},{"id":"c699e423-4062-4ee8-be4c-ff944e62ed4e","keyword":"三阶色散","originalKeyword":"三阶色散"}],"language":"zh","publisherId":"lzdzxb200904021","title":"自<span style=\"color:red\">傅</span>里叶信号在光纤中的传输特性","volume":"26","year":"2009"},{"abstractinfo":"研究了基于横向剪切干涉仪的<span style=\"color:red\">傅</span>里叶剪切干涉方法,对频域中条纹频谱的分布进行了分析,并着重讨论了在不同强度的湍流效应下,几种滤波器带宽(a=5、6、9、11)对波前复原精度的影响,仿真计算结果表明:为了提高<span style=\"color:red\">傅</span>里叶剪切干涉法的复原精度,滤波器的带宽应该随着湍流效应的逐渐增强而适当地变窄.","authors":[{"authorName":"毕振波","id":"afbeb6a2-8eb4-4269-a43f-6b17e36f42e7","originalAuthorName":"毕振波"},{"authorName":"范承玉","id":"69b2c4a1-e395-4cc4-9f14-6b7630fe8fe0","originalAuthorName":"范承玉"},{"authorName":"黄印博","id":"b2b76cd8-d8de-4217-b786-099bf240072b","originalAuthorName":"黄印博"},{"authorName":"王英俭","id":"d95fa5e0-8215-4b6a-9285-5d590a6facb6","originalAuthorName":"王英俭"}],"doi":"10.3969/j.issn.1007-5461.2006.03.008","fpage":"316","id":"351f9d1e-7f5a-442c-b8ca-676ed813df95","issue":"3","journal":{"abbrevTitle":"LZDZXB","coverImgSrc":"journal/img/cover/LZDZXB.jpg","id":"53","issnPpub":"1007-5461","publisherId":"LZDZXB","title":"量子电子学报   "},"keywords":[{"id":"ef67afc8-f614-4302-921f-b804dc40ad96","keyword":"大气光学","originalKeyword":"大气光学"},{"id":"dd859d21-2b47-4856-82c2-bd0378f4dca1","keyword":"带宽","originalKeyword":"带宽"},{"id":"5f69bbc1-f2c8-4b4b-bfef-cd517ffafafa","keyword":"傅里叶变换","originalKeyword":"傅里叶变换"},{"id":"31ed8007-c9e2-4885-9e02-06bf7a2bbd0c","keyword":"湍流效应","originalKeyword":"湍流效应"}],"language":"zh","publisherId":"lzdzxb200603008","title":"滤波器带宽对<span style=\"color:red\">傅</span>里叶剪切干涉法精度的影响","volume":"23","year":"2006"},{"abstractinfo":"采用<span style=\"color:red\">傅</span>里叶级数有关理论,根据缠绕复合材料内部细观结构的特点,建立了缠绕复合材料刚度预测模型.该模型将缠绕复合材料特征单元的刚度作为一个刚度场,利用二维<span style=\"color:red\">傅</span>里叶级数展开得到描述该刚度场的函数.算例的结果表明,本文中所建立的模型可以预测缠绕复合材料整体刚度特性,同时通过<span style=\"color:red\">傅</span>里叶级数各阶展开项的叠加可以反映材料内部细观结构对缠绕复合材料刚度特性的影响.","authors":[{"authorName":"李俭","id":"5c9a163a-8e20-4d2b-9bd2-6d7f1c09be48","originalAuthorName":"李俭"},{"authorName":"温卫东","id":"b1d1f5a6-a965-4ebc-a45c-d358efe5fcc7","originalAuthorName":"温卫东"},{"authorName":"崔海涛","id":"ca6cefc6-117a-41df-a523-277836d1ac89","originalAuthorName":"崔海涛"}],"doi":"","fpage":"169","id":"62bc2493-08a5-4898-9109-49f98ff44b46","issue":"5","journal":{"abbrevTitle":"FHCLXB","coverImgSrc":"journal/img/cover/FHCLXB.jpg","id":"26","issnPpub":"1000-3851","publisherId":"FHCLXB","title":"复合材料学报"},"keywords":[{"id":"63fb7dd7-9d46-4f6e-b9b2-171cb6ee7229","keyword":"缠绕","originalKeyword":"缠绕"},{"id":"ddffdea1-691f-4cd8-aa4a-95a45d946ed0","keyword":"复合材料","originalKeyword":"复合材料"},{"id":"ea9399a7-c918-46af-a357-2faa400d5354","keyword":"刚度","originalKeyword":"刚度"},{"id":"02a94a08-68d9-4fa0-ba95-124bc33db514","keyword":"预测模型","originalKeyword":"预测模型"},{"id":"eb47b871-ce60-4c4c-80ee-6f8b4a73f1d8","keyword":"<span style=\"color:red\">傅</span>里叶级数","originalKeyword":"傅里叶级数"}],"language":"zh","publisherId":"fhclxb200805028","title":"基于<span style=\"color:red\">傅</span>里叶级数的缠绕复合材料刚度预测方法","volume":"25","year":"2008"},{"abstractinfo":"用分步傅里叶变换方法数值求解非线性薛定谔方程,研究了一阶自<span style=\"color:red\">傅</span>里叶光孤子信号在光纤传输中的相互作用特性,证明了算法内部不存在理论误差.数值模拟结果表明:1)一阶自<span style=\"color:red\">傅</span>里叶孤子对中的相互作用表现不同于一阶标准孤子对,它类似于二阶或准二阶孤子之间的相互作用特性.两孤子经历一段周期性的相互吸引后,出现强烈的相互排斥.2)孤子相互作用特性不足以用孤子的阶去区分或分类,在同一阶的孤子中,不同的脉宽对孤子的相互作用有显著不同的影响.3)微弱的三阶色散效应有利于抑制一阶自<span style=\"color:red\">傅</span>里叶孤子间的相互作用.","authors":[{"authorName":"殷德京","id":"19ff89d9-ea5a-430c-a26b-cef288af1fb5","originalAuthorName":"殷德京"}],"doi":"10.3969/j.issn.1007-5461.2012.06.014","fpage":"741","id":"9400e358-5fb0-4032-b477-61861159faa1","issue":"6","journal":{"abbrevTitle":"LZDZXB","coverImgSrc":"journal/img/cover/LZDZXB.jpg","id":"53","issnPpub":"1007-5461","publisherId":"LZDZXB","title":"量子电子学报   "},"keywords":[{"id":"6913d0e1-9cf4-4a5b-b894-acf2fb589190","keyword":"纤维与波导光学","originalKeyword":"纤维与波导光学"},{"id":"8cbdc7bc-5dd5-469e-b94d-7ec2b3d3173e","keyword":"自<span style=\"color:red\">傅</span>里叶孤子","originalKeyword":"自傅里叶孤子"},{"id":"81570af2-6290-44c1-90cf-f774a635cb30","keyword":"分步傅里叶变换方法","originalKeyword":"分步傅里叶变换方法"},{"id":"bb330cd0-a44b-4e2b-ad73-60db1386a1b6","keyword":"相互作用","originalKeyword":"相互作用"},{"id":"4cb46a27-10f8-41c8-b16e-a0f9568afcfb","keyword":"三阶色散","originalKeyword":"三阶色散"}],"language":"zh","publisherId":"lzdzxb201206014","title":"自<span style=\"color:red\">傅</span>里叶光孤子的相互作用特性","volume":"29","year":"2012"},{"abstractinfo":"在对<span style=\"color:red\">傅</span>里叶红外光谱仪与传统的色散型光谱分析仪进行比较的基础上,综述了基于该装置的高温红外光谱发射率测量技术的国内外发展现状.在详细介绍各具特色的装置结构、工作原理、测量温度范围和测量水平的同时,评述了这项技术的特点和局限性,并对其未来发展趋势进行了展望.","authors":[{"authorName":"何小瓦","id":"88a187ff-b6ca-4419-80da-e1d6aaffb772","originalAuthorName":"何小瓦"},{"authorName":"戴景民","id":"3e1a3583-095d-49ec-84bd-ebc53c34508d","originalAuthorName":"戴景民"},{"authorName":"辛春锁","id":"7de618cc-d2f7-4bee-97b8-02010f019442","originalAuthorName":"辛春锁"},{"authorName":"王宗伟","id":"78a30c8f-b5ff-4620-addd-1f47d961bc30","originalAuthorName":"王宗伟"},{"authorName":"徐辉","id":"93d23d4b-c176-45f2-b01b-576c94024488","originalAuthorName":"徐辉"}],"doi":"10.3969/j.issn.1007-2330.2007.05.004","fpage":"13","id":"54d2d3b4-8e16-4bfa-a77e-1fa02d85bb5c","issue":"5","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":"805568c2-060e-4e13-b799-6d103a502061","keyword":"光谱发射率","originalKeyword":"光谱发射率"},{"id":"dcb251de-0a8e-4dd7-a2ca-8a76129f1e15","keyword":"发射率测量","originalKeyword":"发射率测量"},{"id":"96d0bca4-9a7c-4ae7-8549-fe4355995fa4","keyword":"高温环境","originalKeyword":"高温环境"},{"id":"f4f99223-2f7e-4131-a66f-6b5d57bbf0e8","keyword":"FT-IR","originalKeyword":"FT-IR"}],"language":"zh","publisherId":"yhclgy200705004","title":"基于<span style=\"color:red\">傅</span>里叶光谱仪在高温环境下材料光谱发射率测试技术","volume":"37","year":"2007"},{"abstractinfo":"利用XRD线形<span style=\"color:red\">傅</span>氏分析方法定量分析TA15合金在750、800和925℃热压缩变形后的位错亚结构.结果表明:利用 XRD 线性<span style=\"color:red\">傅</span>氏分析的方法可以比较方便地定量表征位错信息;位错类型主要为基面(0002)、柱面(1010)和锥面(1011)型位错.在750℃、1s-1变形条件下,随应变量的增加,直到60%变形量时,位错密度仍在增加.而在800℃、1s-1变形条件下,位错密度先增加后降低.各变形条件下位错密度均在1010～1011cm-2的范围:750℃变形后,各晶面的位错密度随应变量增加而增加,但是基面(0002)和锥面(1011)位错随应变量的增加的速度更快,说明此温度下基面和锥面位错更易滑移:800℃变形后锥面位错密度随着应变量增加稍有增加,而柱面(1010)和基面(0002)的变化很大.","authors":[{"authorName":"刘勇","id":"f9f872bc-2a74-4157-8f74-b185563f6efc","originalAuthorName":"刘勇"},{"authorName":"朱景川","id":"a01988ff-8bdf-4db2-81d2-083950cdceaa","originalAuthorName":"朱景川"},{"authorName":"王洋","id":"333a6294-16cd-4bf5-8449-c7bcb6ad76bc","originalAuthorName":"王洋"},{"authorName":"占家军","id":"ca7da949-5761-458d-9904-5736f7341861","originalAuthorName":"占家军"}],"doi":"","fpage":"1505","id":"164ca2f6-a1ab-4b53-894f-c5d799bdb5fb","issue":"9","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":"a521d85d-e71c-4f0e-8a91-bb4b2d729fd0","keyword":"TA15合金","originalKeyword":"TA15合金"},{"id":"c5c93aed-4d20-40f0-9592-bcae56bdf2f9","keyword":"热压缩变形","originalKeyword":"热压缩变形"},{"id":"d6345368-b954-4b85-9cf7-2ce039992eb9","keyword":"XRD线性<span style=\"color:red\">傅</span>氏分析方法","originalKeyword":"XRD线性傅氏分析方法"},{"id":"76906d41-2c9b-42ec-950d-744047239ccb","keyword":"位错","originalKeyword":"位错"}],"language":"zh","publisherId":"xyjsclygc200809001","title":"XRD线形<span style=\"color:red\">傅</span>氏分析方法研究TA15合金热压缩变形后的位错","volume":"37","year":"2008"}],"totalpage":71,"totalrecord":705}