{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"利用在束实验产生具有β+ / EC衰变性质核素176,178Ir,分析了在束实验条件下获得的γ-γ符合数据,识别出了176Os的4条新能级和13条新γ跃迁、178Os的5条新能级和14条新γ跃迁.籍助氦喷嘴快速带传输系统,进一步对176Ir的β+ / EC衰变进行了测量,在确认在束测量新γ射线的同时建议了176Ir的一个低自旋同核异能态.通过两准粒子耦合的半经验计算,建议了176,178Ir基态及同核异能态的组态.","authors":[{"authorName":"王华磊","id":"b60f3b54-eab4-4607-9569-3fdc3e7120cb","originalAuthorName":"王华磊"},{"authorName":"张玉虎","id":"6b1085ec-3750-4fc3-b338-96cb23590cbe","originalAuthorName":"张玉虎"},{"authorName":"周小红","id":"67f300ae-7639-4a54-b7d2-24afdbf74071","originalAuthorName":"周小红"},{"authorName":"郭应祥","id":"6391f1db-1e3d-44da-b17e-32566c7a6829","originalAuthorName":"郭应祥"},{"authorName":"雷祥国","id":"d7faf153-8dbe-44dd-a8ab-024b46de80d9","originalAuthorName":"雷祥国"},{"authorName":"徐树威","id":"7bd3a8c5-7890-4cb2-a6f2-7a5333b04d55","originalAuthorName":"徐树威"},{"authorName":"谢元祥","id":"0564a43d-3752-446b-96f1-b657ddaa56fa","originalAuthorName":"谢元祥"},{"authorName":"郑勇","id":"1ac93a87-9ea0-4d71-8272-5aadacbcc77e","originalAuthorName":"郑勇"},{"authorName":"柳敏良","id":"56a6d532-53a7-4c13-a30f-3fb8ccddfb7d","originalAuthorName":"柳敏良"},{"authorName":"邢烨炳","id":"3854c1ad-acde-44df-9032-4652520ec293","originalAuthorName":"邢烨炳"},{"authorName":"谢成营","id":"4c5ff4a1-6704-4113-91b8-3c6826c1a348","originalAuthorName":"谢成营"},{"authorName":"宋立涛","id":"2e11700a-6e7f-4832-8219-f303fb744d5a","originalAuthorName":"宋立涛"},{"authorName":"郭文涛","id":"f4806212-573e-44cd-afe0-08983c9c5c85","originalAuthorName":"郭文涛"},{"authorName":"T.Hayakawa","id":"39e303b6-9c7e-45f0-8ffc-5afc620b4b9f","originalAuthorName":"T.Hayakawa"},{"authorName":"<span style=\"color:red\">M</span>.Oshima","id":"bd8301b4-7a81-4d4b-87e3-ff78c2a6ad89","originalAuthorName":"M.Oshima"},{"authorName":"Y.Toh","id":"63ed5525-7f65-48b1-91e9-413300b5f2c6","originalAuthorName":"Y.Toh"},{"authorName":"J.Katakura","id":"4f616d00-71ea-4569-b60d-515c0c4dc67b","originalAuthorName":"J.Katakura"},{"authorName":"Y.Hatssukawa","id":"02b7ca0a-4cb2-4dc6-9944-b44f749e845e","originalAuthorName":"Y.Hatssukawa"},{"authorName":"<span style=\"color:red\">M.Matsuda</span>","id":"51ace7bf-97c8-4512-87fe-dd95e5369614","originalAuthorName":"M.Matsuda"},{"authorName":"N.Shinohara","id":"e8c42c95-cf06-4392-8e42-206b12d31d98","originalAuthorName":"N.Shinohara"},{"authorName":"T.Ishii","id":"f7483a01-6d65-495a-9870-8486f2b32b03","originalAuthorName":"T.Ishii"},{"authorName":"H.Kusakari","id":"c20d41ed-fca4-4ceb-a652-be85079f3670","originalAuthorName":"H.Kusakari"},{"authorName":"<span style=\"color:red\">M</span>.Sugawara","id":"fd173f9d-6314-4d52-8e74-49be0a12bd05","originalAuthorName":"M.Sugawara"},{"authorName":"T.Komatsubara","id":"13ddda9b-cf93-4657-bc1a-93cc44008ac4","originalAuthorName":"T.Komatsubara"}],"doi":"10.3969/j.issn.1007-4627.2006.01.004","fpage":"13","id":"6451aa6b-4938-41a0-bd7e-a158fc405828","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":"713a5aca-46ea-43bb-9097-3d35c715b212","keyword":"低位能级纲图","originalKeyword":"低位能级纲图"},{"id":"e6bee87e-1714-4bd8-86c8-9f6378e433a7","keyword":"在束测量","originalKeyword":"在束测量"},{"id":"67e1f243-000e-46c4-9211-00e4376ed2dd","keyword":"半衰期","originalKeyword":"半衰期"}],"language":"zh","publisherId":"yzhwlpl200601004","title":"176,178Os新低位激发态的识别","volume":"23","year":"2006"},{"abstractinfo":"超塑性<span style=\"color:red\">m</span>-δ关系曲线可以分为<span style=\"color:red\">m</span>_L=<span style=\"color:red\">m</span>_(max)和<span style=\"color:red\">m</span>_L=<span style=\"color:red\">m</span>_(min)两大类型。均可由下面的C.L.(刘勤)<span style=\"color:red\">m</span>-σ方程表示:σ(%)=〔cε~(<span style=\"color:red\">m-m</span>_0)-1〕×100当σ=σ_0=0时,<span style=\"color:red\">m</span>=<span style=\"color:red\">m</span>_0≠0,C=C_0=κ_0/κ_0=1。当σ=σ_1(σ_(11),σ_(12),σ_(13),…,)时,<span style=\"color:red\">m</span>=<span style=\"color:red\">m</span>_1(<span style=\"color:red\">m</span>_(11),<span style=\"color:red\">m</span>_(12),<span style=\"color:red\">m</span>_(13),…),C=C_1(C_(11),C_(12),C_(13),…)=κ_1(κ_(11),κ_(12),κ_(13),…)/κ_0,当σ=σ_F时,<span style=\"color:red\">m</span>=<span style=\"color:red\">m</span>_F,C=C_F=κ_F/κ_0。对C 值进行“规划”,得到的C_1~(σ_O-σ_L)-(<span style=\"color:red\">m</span>_L=<span style=\"color:red\">m</span>_(max)),C_2~(σ_F-σ_L)-(<span style=\"color:red\">m</span>_L=<span style=\"color:red\">m</span>_(min)),C_3~(<span style=\"color:red\">m_0-m</span>_L)-(<span style=\"color:red\">m</span>_L=<span style=\"color:red\">m</span>_(max)和C_4~(<span style=\"color:red\">m_F-m</span>_L)-(<span style=\"color:red\">m</span>_L=<span style=\"color:red\">m</span>_(min))四种类型的“规划”方程分别对<span style=\"color:red\">m</span>_L=<span style=\"color:red\">m</span>_(max)和<span style=\"color:red\">m</span>_L=<span style=\"color:red\">m</span>_(min)型<span style=\"color:red\">m</span>-σ曲线适用。若<span style=\"color:red\">m</span>-σ曲线属简单的下降式,C 及其“规划”值均可近似地取1。否则,C-σ关系是应加以研究的问题。<span style=\"color:red\">m</span> 和k 值对σ值的效应可以分为动态(直接)和静态(间接)两种。最后的σ值是两种效应的综合结果。(注:<span style=\"color:red\">m</span> 和κ值见基本方程σ=κε~<span style=\"color:red\">m</span>)","authors":[{"authorName":"刘勤","id":"548de7f9-991f-4241-847d-cdc61297a458","originalAuthorName":"刘勤"},{"authorName":"周善佑","id":"3e155d7e-5bb1-4dee-9ddd-fdc10bc50dd9","originalAuthorName":"周善佑"}],"categoryName":"|","doi":"","fpage":"1","id":"81122113-fa5b-4a2b-a387-1f5fc6f8a5f1","issue":"5","journal":{"abbrevTitle":"CLYJXB","coverImgSrc":"journal/img/cover/CLYJXB.jpg","id":"16","issnPpub":"1005-3093","publisherId":"CLYJXB","title":"材料研究学报"},"keywords":[],"language":"zh","publisherId":"1005-3093_1988_5_7","title":"超塑性 <span style=\"color:red\">m</span>-δ关系","volume":"2","year":"1988"},{"abstractinfo":"研究了<span style=\"color:red\">m</span>(<span style=\"color:red\">M</span>)/<span style=\"color:red\">m</span>(P)比值对磷酸镁水泥干燥收缩行为的影响，采用温度记录仪、压汞仪、X 射线衍射仪、扫描电镜及能谱仪等分析手段探讨了<span style=\"color:red\">m</span>(<span style=\"color:red\">M</span>)/<span style=\"color:red\">m</span>(P)比值对磷酸镁水泥干燥收缩的作用机理。结果表明，随着<span style=\"color:red\">m</span>(<span style=\"color:red\">M</span>)/<span style=\"color:red\">m</span>(P)比值的增大，磷酸镁水泥水化初期的膨胀量以及干燥收缩减小；水化8 h左右水泥开始收缩，龄期达到20 d左右收缩趋于稳定；磷酸镁水泥收缩量的减少，是由于<span style=\"color:red\">m</span>(<span style=\"color:red\">M</span>)/<span style=\"color:red\">m</span>(P)比值的增大导致磷酸镁水泥水化温度降低，孔隙率增大，水化产物MgKPO4?6 H2 O 减少，水化产物结构趋于疏松。","authors":[{"authorName":"戴丰乐","id":"48e92b6c-2794-4e0d-b116-409bbaa895fa","originalAuthorName":"戴丰乐"},{"authorName":"齐召庆","id":"74f2e0d9-f4ea-486f-b705-5476bd04d2c7","originalAuthorName":"齐召庆"},{"authorName":"汪宏涛","id":"0f9d3782-5775-41a5-95d3-d4b6be91b00c","originalAuthorName":"汪宏涛"},{"authorName":"姜自超","id":"56cabcbe-908f-465e-b64b-8b1fb9e48691","originalAuthorName":"姜自超"},{"authorName":"张时豪","id":"ca998013-8fbb-461e-b1d4-cbe49491c8fb","originalAuthorName":"张时豪"},{"authorName":"丁建华","id":"11929a56-dc74-4aa0-9111-9f9053cc5074","originalAuthorName":"丁建华"}],"doi":"10.3969/j.issn.1001-9731.2016.12.022","fpage":"12134","id":"b6df2ad0-156a-4032-b987-1432a633f8bb","issue":"12","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"6a45698d-745a-4b34-af1c-b707c57dd4df","keyword":"磷酸镁水泥","originalKeyword":"磷酸镁水泥"},{"id":"69123d77-227e-47a7-82b3-9fcbc48883e0","keyword":"干燥收缩","originalKeyword":"干燥收缩"},{"id":"517e18b7-3f95-4b20-af4e-8dd4a8b5f600","keyword":"<span style=\"color:red\">m</span>(<span style=\"color:red\">M</span>)/<span style=\"color:red\">m</span>(P)比值","originalKeyword":"m(M)/m(P)比值"}],"language":"zh","publisherId":"gncl201612022","title":"<span style=\"color:red\">m</span>（<span style=\"color:red\">M</span>）/<span style=\"color:red\">m</span>（P）比值对磷酸镁水泥干燥收缩的影响及机理研究?","volume":"47","year":"2016"},{"abstractinfo":"采用改进的非接触式混凝土收缩测定仪及标靶,研究了<span style=\"color:red\">m</span>(<span style=\"color:red\">M</span>)/<span style=\"color:red\">m</span>(P)比值(MgO与KH2PO4的质量比)对磷酸镁水泥石自收缩行为的影响,运用八通道微量量热仪、压汞仪、X射线衍射仪、扫描电子显微镜及能谱仪等分析手段,分析了<span style=\"color:red\">m</span>(<span style=\"color:red\">M</span>)/<span style=\"color:red\">m</span>(P)比值对磷酸镁水泥石自收缩的作用机理.结果表明,磷酸镁水泥石的自收缩呈现出3个阶段的特征,即早期的迅速收缩阶段、微膨胀阶段、收缩缓慢发展阶段.随着<span style=\"color:red\">m</span>(<span style=\"color:red\">M</span>)/<span style=\"color:red\">m</span>(P)比值的增大,由于磷酸镁水泥石的水化放热量降低,水泥石内部孔隙率增大,水化产物结晶度降低,水泥石结构疏松,所以,自收缩率减小.","authors":[{"authorName":"齐召庆","id":"aa06bbfa-b638-4cab-aff4-2d625b1078ec","originalAuthorName":"齐召庆"},{"authorName":"汪宏涛","id":"35a45919-5c94-4043-88b3-3fa35590df5f","originalAuthorName":"汪宏涛"},{"authorName":"薛明","id":"a72bb669-bc19-4cc7-a3f4-c80f3d33c8cd","originalAuthorName":"薛明"}],"doi":"10.3969/j.issn.1001-9731.2016.02.010","fpage":"2046","id":"3d4b3944-8192-4c0d-9eb1-cdf2695a7326","issue":"2","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"4273c763-03a2-4853-89e4-9d7806841ad0","keyword":"磷酸镁水泥","originalKeyword":"磷酸镁水泥"},{"id":"a3db27c1-a4bb-43ac-9b40-a2b5764764ca","keyword":"自收缩","originalKeyword":"自收缩"},{"id":"012eda38-f5ec-4f34-ac08-e641bd02a682","keyword":"<span style=\"color:red\">m</span>(<span style=\"color:red\">M</span>)/<span style=\"color:red\">m</span>(P)比值","originalKeyword":"m(M)/m(P)比值"}],"language":"zh","publisherId":"gncl201602010","title":"<span style=\"color:red\">m</span>(<span style=\"color:red\">M</span>)/<span style=\"color:red\">m</span>(P)比值对磷酸镁水泥石自收缩的影响及机理研究","volume":"47","year":"2016"},{"abstractinfo":"Magnetic stripe is one of the major applications of magnetic materials. As a key component of the present card technologies magnetic stripes play reliable components for electronic data interchange in worldwide electronic payment systems such as financial cards, transit tickets and phone cards, etc. Magnetic stripes are available in various coercivity materials, widths, lengths, structures and colors with each types of transferable, lamination and pressure sensitive magnetic tapes of Deuton-<span style=\"color:red\">M</span>. Manufacturing process, structure and characteristics of Deuton-<span style=\"color:red\">M</span> magnetic tape and sheet are described.","authors":[{"authorName":"Tesshu Miyahara","id":"2ffad82c-4d28-4fec-af4e-b93ca3c990c0","originalAuthorName":"Tesshu Miyahara"}],"categoryName":"|","doi":"","fpage":"228","id":"5d803199-344c-4d27-ad7d-9bd4299b2511","issue":"2","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_2000_2_11","title":"Deuton-<span style=\"color:red\">M</span> magnetic tapes and sheets for cards","volume":"16","year":"2000"},{"abstractinfo":"为了得到2.7 μ<span style=\"color:red\">m</span>波段可调谐激光辐射,设计了信号光单谐振荡KTP光参量振荡器(OPO),给出了KTP OPO II(B)类相位匹配方式下的角度调谐曲线、有效非线性系数.KTP晶体切割角为θ=62°,ψ=0°,有效非线性系数为-2.97 pm/V.利用该KTP OPO实现了2.6～2.8 μ<span style=\"color:red\">m</span>波段范围可调谐激光输出,用脉宽为16 ns的基模高斯光束1.064 μ<span style=\"color:red\">m</span>激光泵浦得到了最大能量578 μJ,能量转换效率达1.7%.","authors":[{"authorName":"卞进田","id":"33ea5b5d-8e49-4917-85fa-f19b60ab3946","originalAuthorName":"卞进田"},{"authorName":"孙晓泉","id":"44d32281-b079-4203-8d5f-9ec19648b791","originalAuthorName":"孙晓泉"},{"authorName":"聂劲松","id":"302acbc8-5bf7-4374-807a-72bb3bd65161","originalAuthorName":"聂劲松"}],"doi":"10.3969/j.issn.1007-5461.2008.02.019","fpage":"226","id":"69733e9b-7dbf-4288-90c5-7ada09e1d2a7","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":"27cd9f91-8a79-4a22-aa3e-61f3c96cdd52","keyword":"非线性光学","originalKeyword":"非线性光学"},{"id":"0198dd46-a74d-4848-b33d-3446b8c7a007","keyword":"可调谐红外激光","originalKeyword":"可调谐红外激光"},{"id":"d251a99e-2f29-475d-b766-5b5ccf742713","keyword":"单谐振光参量振荡器","originalKeyword":"单谐振光参量振荡器"},{"id":"1eccf314-f727-424f-ae3c-e708ed333c29","keyword":"KTP","originalKeyword":"KTP"},{"id":"28f29420-8da5-426b-b20c-95f684fe9bc0","keyword":"角度调谐","originalKeyword":"角度调谐"},{"id":"bfd118a5-2eb0-4881-9c32-9b44b6783f40","keyword":"相位匹配","originalKeyword":"相位匹配"}],"language":"zh","publisherId":"lzdzxb200802019","title":"2.6～2.8μ<span style=\"color:red\">m</span> KTP OPO实验研究","volume":"25","year":"2008"},{"abstractinfo":"针对φ3.2<span style=\"color:red\">m</span>×3.1<span style=\"color:red\">m</span>球磨机齿轮轴损坏的四种形式,分别进行分析,提出了解决方案.","authors":[{"authorName":"刘险峰","id":"da9f5095-8e87-4163-9369-0661e4b3e9be","originalAuthorName":"刘险峰"}],"doi":"10.3969/j.issn.1000-6826.2007.05.020","fpage":"57","id":"4ca540b4-2876-47b6-872d-af13735fade9","issue":"5","journal":{"abbrevTitle":"JSSJ","coverImgSrc":"journal/img/cover/3abe017a-2574-4821-8152-4ae974ef0471.jpg","id":"47","issnPpub":"1000-6826","publisherId":"JSSJ","title":"金属世界"},"keywords":[{"id":"84ac976a-e2dd-4d3e-b046-b657428cc1b8","keyword":"球磨机齿轮轴","originalKeyword":"球磨机齿轮轴"},{"id":"4d7f2093-49dd-4ce8-8ce5-4741cf91e329","keyword":"断裂","originalKeyword":"断裂"},{"id":"ad611a23-58ae-4852-abd0-bbbd1ba1da04","keyword":"磨损","originalKeyword":"磨损"},{"id":"b1e2198e-5af3-49f8-b4f0-0e1a9791345c","keyword":"解决方案","originalKeyword":"解决方案"}],"language":"zh","publisherId":"jssj200705020","title":"φ3.2<span style=\"color:red\">m</span>×3.1<span style=\"color:red\">m</span>球磨机齿轮轴损坏分析及解决方案","volume":"","year":"2007"},{"abstractinfo":"We investigated the stable (0001) surfaces of <span style=\"color:red\">M</span>(2)AlC (<span style=\"color:red\">M</span> = Ti, V and Cr) using the first-principles plane-wave pseudopotential total energy method. Four possible (0001) terminations were considered by breaking the <span style=\"color:red\">M</span>-Al and <span style=\"color:red\">M</span>-C bonds. The corresponding surface energies were calculated and compared. The Al-and <span style=\"color:red\">M</span>(C)-terminated (0001) surfaces demonstrated better stability than the C- and <span style=\"color:red\">M</span>(Al)-terminated surfaces by their much lower surface energies. In addition, the stability of surfaces was predicted under various chemical environments as a function of chemical potentials. We further investigated the character of surface relaxations. The electronic structures of the stable Al- and <span style=\"color:red\">M</span>(C)-terminated surfaces were analyzed.","authors":[],"categoryName":"|","doi":"","fpage":"","id":"c0893659-ce4b-414e-a93a-111e4528fd79","issue":"22","journal":{"abbrevTitle":"JOPM","id":"f0e359df-48a6-4a7f-b16d-2389d3e793ee","issnPpub":"0953-8984","publisherId":"JOPM","title":"Journal of Physics-Condensed Matter"},"keywords":[{"id":"cfefea4d-875f-4a08-a374-3e22aaf64de9","keyword":"ab-initio calculations;ti3sic2 thin-films;electronic-structure;elastic stiffness;al;deposition;cr2alc;simulation;adhesion;solids","originalKeyword":"ab-initio calculations;ti3sic2 thin-films;electronic-structure;elastic stiffness;al;deposition;cr2alc;simulation;adhesion;solids"}],"language":"en","publisherId":"0953-8984_2008_22_1","title":"Stable <span style=\"color:red\">M</span>(2)AlC(0001) surfaces (<span style=\"color:red\">M</span> = Ti, V and Cr) by first-principles investigation","volume":"20","year":"2008"},{"abstractinfo":"本文主要介绍了承德建龙炼铁厂580<span style=\"color:red\">m</span>3高炉开炉前的准备工作、开炉方案的确定以及开炉生产实践等.本次开炉采用了热风点火、全焦开炉等当前新方法,通过制订合理的烘炉和开炉方案,高炉开炉取得圆满成功,生产水平快速提高.","authors":[{"authorName":"王少红","id":"9f346f1b-f093-43c1-b4f0-868418ef1f64","originalAuthorName":"王少红"},{"authorName":"刘志勇","id":"750da4a0-2743-4bc3-a8e7-35bd4692c89d","originalAuthorName":"刘志勇"}],"doi":"10.3969/j.issn.1000-6826.2009.01.005","fpage":"10","id":"8d1b2c23-e4be-40a4-9e5a-67108571b84b","issue":"1","journal":{"abbrevTitle":"JSSJ","coverImgSrc":"journal/img/cover/3abe017a-2574-4821-8152-4ae974ef0471.jpg","id":"47","issnPpub":"1000-6826","publisherId":"JSSJ","title":"金属世界"},"keywords":[{"id":"c13a3bf6-de9d-431b-b12e-548d9b400eb0","keyword":"高炉","originalKeyword":"高炉"},{"id":"88649fda-a8ae-4587-aeff-b4c43a402f8a","keyword":"开炉","originalKeyword":"开炉"},{"id":"df6c3e9e-2933-40c6-b9d1-d9e8685842a7","keyword":"烘炉","originalKeyword":"烘炉"},{"id":"0762314c-146a-4599-a6b0-3111793ed85b","keyword":"效果","originalKeyword":"效果"}],"language":"zh","publisherId":"jssj200901005","title":"580<span style=\"color:red\">m</span>3高炉开炉实践","volume":"","year":"2009"},{"abstractinfo":"本文报道了我所生长的掺钕钨酸钾钆(KGW)晶体的脉冲激光特性.当用氙闪光灯泵浦时,尺寸为φ3.4 mm×24 mm的KGW激光棒,最大激光输出为每个脉冲358.4mJ,总效率为1.7%,斜率效率为3.3%,波长为1.067μ<span style=\"color:red\">m</span>.实验证明,KGW是一种很有前途的小型激光器工作物质.","authors":[{"authorName":"邱闽旺","id":"602a396e-2757-449c-b731-5538dfa0405a","originalAuthorName":"邱闽旺"},{"authorName":"涂朝阳","id":"04285b4b-1227-4497-924d-de46593cb1c9","originalAuthorName":"涂朝阳"},{"authorName":"李坚富","id":"ae321b20-5e65-4592-bd7b-87ea08b1cb2d","originalAuthorName":"李坚富"},{"authorName":"黄奕川","id":"590e432a-7721-4926-970d-1daadac5f272","originalAuthorName":"黄奕川"},{"authorName":"汪爱栋","id":"fc7eb4a7-d9c3-4e3e-8f85-173a33adb961","originalAuthorName":"汪爱栋"},{"authorName":"唐鼎元","id":"a730ad4c-5cc1-4c6f-aa2f-81d7702be1e3","originalAuthorName":"唐鼎元"},{"authorName":"王元康","id":"5c25121b-9917-4da7-991a-39bf30235733","originalAuthorName":"王元康"}],"doi":"10.3969/j.issn.1007-5461.2001.04.012","fpage":"340","id":"068cb591-a560-4445-b01a-01ed8770d424","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":"fc97e00d-e678-47fc-be91-fe8fbeccb91c","keyword":"掺钕钨酸钾钆(KGW)晶体","originalKeyword":"掺钕钨酸钾钆(KGW)晶体"},{"id":"b5603346-e582-46c4-8a0d-8cefafc5db13","keyword":"1.067 μ<span style=\"color:red\">m</span>激光","originalKeyword":"1.067 μm激光"}],"language":"zh","publisherId":"lzdzxb200104012","title":"KGW晶体1.067μ<span style=\"color:red\">m</span>激光特性研究","volume":"18","year":"2001"}],"totalpage":2362,"totalrecord":23615}