{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"精确求解了自旋-1/2粒子在旋转磁场下的Bloch方程和Schrodinger方程.用此问题的循环解,得到了Aharonov-Anandan(AA)几何相和动力学相的解析结果,并用正交态方法构造了具有和乐几何量子计算优点的非绝热几何量子门.基于一般的SU(2)循环演化条件,还构造了只依赖轨道的绕数和扭结数的普适拓扑量子门.最后建议用非对称的约瑟夫森结纳米电路实现所构造的各种量子门.","authors":[{"authorName":"高玉梅","id":"469c2ef4-d1a3-4181-bfb8-00e7e841582b","originalAuthorName":"高玉梅"},{"authorName":"胡连","id":"9526d2bb-5046-40c9-818b-003dcd63de0c","originalAuthorName":"胡连"}],"doi":"10.3969/j.issn.1007-5461.2006.02.012","fpage":"183","id":"4c184475-6cc3-4d58-a49f-2b4825da1dfe","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":"9741e969-41c1-48b8-be11-4357d736a2e7","keyword":"量子光学","originalKeyword":"量子光学"},{"id":"3a8d5cb3-c7d6-4954-813e-0f8b66befb9d","keyword":"非绝热几何量子计算","originalKeyword":"非绝热几何量子计算"},{"id":"786a5b07-96c3-4817-a1d7-f98a3c48cda5","keyword":"正交态方法","originalKeyword":"正交态方法"},{"id":"b85108d8-d0e1-47d5-bd06-efef0e6f8216","keyword":"<span style=\"color:red\">准</span><span style=\"color:red\">平行</span><span style=\"color:red\">传输</span>","originalKeyword":"准平行传输"},{"id":"c8ebf9f0-d128-4be0-a019-738def6fcad4","keyword":"拓扑量子门","originalKeyword":"拓扑量子门"}],"language":"zh","publisherId":"lzdzxb200602012","title":"非绝热几何量子计算及拓扑量子门","volume":"23","year":"2006"},{"abstractinfo":"利用<span style=\"color:red\">传输</span>矩阵方法,研究了不同偏振情形下,电磁波在正负折射率媒质构成的Fibonacci<span style=\"color:red\">准</span>周期超晶格中的传播规律.结果表明:随着入射角的增加,S偏振时的禁带有加宽趋势,但在一定角度时消失;P偏振时的禁带则始终加宽,且出现了全向带隙.还进一步研究了引入缺陷后的偏振特性,并通过将有缺陷的Fibonacci<span style=\"color:red\">准</span>周期超晶格重叠获得了在某一偏振下全反射而在另一偏振下全透射的良好特性.这将在微波器件和光学器件中有广泛应用.","authors":[{"authorName":"伍清萍","id":"27db6f63-6463-46a1-a7d0-5c276b9ae6d1","originalAuthorName":"伍清萍"},{"authorName":"刘正方","id":"4781e92d-9e32-467a-9c3f-bc7b02c8c208","originalAuthorName":"刘正方"},{"authorName":"陈爱喜","id":"4309efb9-ff03-409d-b029-46f5e96fddca","originalAuthorName":"陈爱喜"}],"doi":"10.3969/j.issn.1007-5461.2008.01.020","fpage":"105","id":"cfb18170-22ee-4923-8c35-ecfc782d6cad","issue":"1","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":"ddb5dd0c-0a54-4ca3-8f40-adb1a5ac2847","keyword":"纤维与波导光学","originalKeyword":"纤维与波导光学"},{"id":"e0179f4d-caeb-4a48-91be-5cb617d09cd8","keyword":"负折射率介质","originalKeyword":"负折射率介质"},{"id":"e841bf64-ea62-483b-9499-9f7982f2da27","keyword":"Fibonacci<span style=\"color:red\">准</span>周期超晶格","originalKeyword":"Fibonacci准周期超晶格"},{"id":"673b2b31-c848-4083-8564-ee3654905598","keyword":"偏振","originalKeyword":"偏振"},{"id":"c27408d6-1d9f-4a3a-9611-0e95446b54b4","keyword":"透射系数","originalKeyword":"透射系数"}],"language":"zh","publisherId":"lzdzxb200801020","title":"不同偏振下Fibonacci<span style=\"color:red\">准</span>周期超晶格的<span style=\"color:red\">传输</span>特性","volume":"25","year":"2008"},{"abstractinfo":"建立了氮极性(N-polar)GaN基HEMT器件的<span style=\"color:red\">准</span>二维(Quasi-2-D)电荷<span style=\"color:red\">传输</span>模型,仿真研究了N-polar GaN基HEMT的直流特性.仿真结果表明,不同的极化效应会对输出特性曲线和转移特性曲线产生不同的影响,考虑自发极化效应(Psp)+压电极化效应(Ppe)、只考虑Ppe和只考虑Psp三种情况下的阈值电压分别为:-3.96 V、-2.29 V和-2.47 V,而其对应的峰值跨导则分别为44 mS/mm、41.2 mS/mm和41.3 mS/mm.该模型为N-polar GaN基HEMT器件仿真提供了理论参考.","authors":[{"authorName":"王现彬","id":"42e1981a-0ef8-457a-9839-803df85e708f","originalAuthorName":"王现彬"},{"authorName":"赵正平","id":"4c0acc8c-a23f-423b-9918-3de1f247494e","originalAuthorName":"赵正平"}],"doi":"10.11896/j.issn.1005-023X.2016.06.032","fpage":"133","id":"8db4603e-8378-432b-8b21-fac7282ab568","issue":"6","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"4cadb681-433d-46d8-b4a8-ec4f5ae978d1","keyword":"N极性","originalKeyword":"N极性"},{"id":"f9c251d3-9e81-4749-aa97-8da906cd87c0","keyword":"高电子迁移率晶体管","originalKeyword":"高电子迁移率晶体管"},{"id":"b3e95c43-d2d2-4b2d-86a9-003901d6ae63","keyword":"极化效应","originalKeyword":"极化效应"},{"id":"8659c8a0-ea23-463c-af19-c80fc2789da9","keyword":"直流特性","originalKeyword":"直流特性"}],"language":"zh","publisherId":"cldb201606033","title":"N-polar GaN基HEMT<span style=\"color:red\">准</span>二维电荷<span style=\"color:red\">传输</span>模型仿真","volume":"30","year":"2016"},{"abstractinfo":"利用实验测量和Monte Carlo模拟的方法,研究了RIBLL的<span style=\"color:red\">传输</span>效率.分析了影响<span style=\"color:red\">传输</span>效率的主要因素,发现碎片的动量分布形式对<span style=\"color:red\">传输</span>效率的模拟结果有重要的影响.另外通过比较,发现大部分碎片<span style=\"color:red\">传输</span>效率的模拟结果稍大于实验测量结果,两者最大相差约几十倍,这可以帮助估算次级束流强度,指导实验设计.","authors":[{"authorName":"章学恒","id":"c82c2d21-e592-40fe-bf37-e9fc3b618223","originalAuthorName":"章学恒"},{"authorName":"孙志宇","id":"f7a7581a-a033-44f2-bf3a-7787831a2e38","originalAuthorName":"孙志宇"},{"authorName":"王猛","id":"f5f5ccd9-9756-4ff1-b6d4-f3264b572c33","originalAuthorName":"王猛"},{"authorName":"陈志强","id":"8611d5a0-e2c2-4209-a9b3-344d1bbd32c8","originalAuthorName":"陈志强"},{"authorName":"胡正国","id":"9e16ff70-3b15-4782-a942-15d2caf8a30b","originalAuthorName":"胡正国"},{"authorName":"王建松","id":"2d1a2dc9-b844-435e-80f4-d4e1dd29e982","originalAuthorName":"王建松"},{"authorName":"毛瑞士","id":"2c6981aa-3a3e-4254-96f2-129eb484dea6","originalAuthorName":"毛瑞士"},{"authorName":"张雪荧","id":"7d1ef53e-b380-4673-a8e7-78c55e72040a","originalAuthorName":"张雪荧"},{"authorName":"赵铁成","id":"9c87bceb-ab0c-436a-a200-d31cd41f61b6","originalAuthorName":"赵铁成"},{"authorName":"李琛","id":"5a8a64be-a983-4694-9310-a3d1b5c37f42","originalAuthorName":"李琛"},{"authorName":"徐瑚珊","id":"e91d2024-c096-4306-be44-69faa6400353","originalAuthorName":"徐瑚珊"},{"authorName":"肖国青","id":"9a423fba-e3f1-4f2b-99b1-1cd225d92a57","originalAuthorName":"肖国青"},{"authorName":"袁小华","id":"698fa213-7d1b-46d1-aa52-c7c0da3ac5e6","originalAuthorName":"袁小华"},{"authorName":"徐志国","id":"e3e64c31-45f6-4150-836e-96772a2c8ff6","originalAuthorName":"徐志国"},{"authorName":"陈若富","id":"e99071a2-b9f3-4bee-9732-c6adafe3f22b","originalAuthorName":"陈若富"},{"authorName":"郭忠言","id":"be3d5f13-20f7-4664-95aa-b318eb6ca29f","originalAuthorName":"郭忠言"},{"authorName":"王玥","id":"8ce2f105-165e-406d-a84c-ea0fa8736262","originalAuthorName":"王玥"},{"authorName":"黄天衡","id":"e4ddf9e4-8a50-4dd8-aff2-6fd1b18e2a62","originalAuthorName":"黄天衡"},{"authorName":"张宏斌","id":"ab590c52-4810-43ce-b0ab-176c046ce053","originalAuthorName":"张宏斌"}],"doi":"","fpage":"203","id":"a16158e4-4023-4d5a-9436-abd42c3ad748","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":"cbde528c-a5e2-48c5-8ce1-afa3cdf6ec2e","keyword":"RIBLL","originalKeyword":"RIBLL"},{"id":"2b516902-7e10-499e-82ba-89030751b69e","keyword":"<span style=\"color:red\">传输</span>效率","originalKeyword":"传输效率"},{"id":"6fc51a2c-9f6d-48a1-a186-41e6111350ca","keyword":"MoCADl","originalKeyword":"MoCADl"},{"id":"03b09bf9-ae9c-4f59-ac40-ff79253b8ba0","keyword":"LISE++","originalKeyword":"LISE++"}],"language":"zh","publisherId":"yzhwlpl200903006","title":"RIBLL<span style=\"color:red\">传输</span>效率研究","volume":"26","year":"2009"},{"abstractinfo":"扫描电镜观察显示胫骨是一种由羟基磷灰石和胶原蛋白组成的生物陶瓷复合材料,其增强相羟基磷灰石<span style=\"color:red\">平行</span>于骨的表面以层状的形式排列.观察也显示这些羟基磷灰石层又是由许多长而薄的羟基磷灰石片所组成,这些羟基磷灰石片也<span style=\"color:red\">平行</span>排列,且其厚度具有纳米的尺度.基于在胫骨中观察到的羟基磷灰石片<span style=\"color:red\">平行</span>纳米结构,建立模型,研究了其最大拔出能.结果表明羟基磷灰石片长而薄的形状以及<span style=\"color:red\">平行</span>排列方式增加了其最大拔出能,进而提高了骨的断裂韧性.","authors":[{"authorName":"陈斌","id":"46475138-69d7-4e42-a78e-db24fcab17aa","originalAuthorName":"陈斌"},{"authorName":"孙士涛","id":"ffccad00-3f7f-47dd-9959-0040f9ec036d","originalAuthorName":"孙士涛"},{"authorName":"彭向和","id":"9aa29e9e-2d19-4c83-9677-748abdd5f26b","originalAuthorName":"彭向和"}],"doi":"10.3969/j.issn.1007-4252.2008.05.018","fpage":"939","id":"a0758361-2049-4e4c-9947-89579d0b5e02","issue":"5","journal":{"abbrevTitle":"GNCLYQJXB","coverImgSrc":"journal/img/cover/GNCLYQJXB.jpg","id":"34","issnPpub":"1007-4252","publisherId":"GNCLYQJXB","title":"功能材料与器件学报   "},"keywords":[{"id":"d69fdaea-a9f0-412a-9d4f-402d9885874a","keyword":"胫骨","originalKeyword":"胫骨"},{"id":"f5ef7c69-24ee-426f-a73c-025699e99433","keyword":"羟基磷灰石片","originalKeyword":"羟基磷灰石片"},{"id":"2dc43689-0400-482c-84f4-94149b57e344","keyword":"纳米<span style=\"color:red\">平行</span>微结构","originalKeyword":"纳米平行微结构"},{"id":"c2ade199-3e34-400f-853e-464d058a4a16","keyword":"最大拔出能","originalKeyword":"最大拔出能"}],"language":"zh","publisherId":"gnclyqjxb200805018","title":"胫骨羟基磷灰石片<span style=\"color:red\">平行</span>纳米结构","volume":"14","year":"2008"},{"abstractinfo":"根据晶界的电阻率大于晶界两侧晶粒的电阻率,提出晶界对<span style=\"color:red\">传输</span>信号影响的电容模型.通过不同温度退火,得到含晶界数不同的铜导线,将含不同晶界数的铜导线制备成标准的高保真同轴电缆,并测量其电容值以及损耗正切值.测量结果表明:导线的电容值以及正切损耗值随晶界数的增加而降低,其数值关系满足关系式.垂直于信号<span style=\"color:red\">传输</span>方向的晶界对<span style=\"color:red\">传输</span>信号的影响显著,而<span style=\"color:red\">平行</span>于<span style=\"color:red\">传输</span>信号的晶界对信号的影响相对弱一些.由于晶界的电容效应,晶界增加<span style=\"color:red\">传输</span>信号的失真度,增加同轴电缆对<span style=\"color:red\">传输</span>信号的衰减量等.","authors":[{"authorName":"陈建","id":"90914665-bd89-4a92-9edf-1a68c96a2bec","originalAuthorName":"陈建"},{"authorName":"严文","id":"5be72452-2b8a-4cf9-8128-954e7e0b6cec","originalAuthorName":"严文"},{"authorName":"范新会","id":"eb08d073-9fa4-4112-bae4-bfbf933054b1","originalAuthorName":"范新会"},{"authorName":"刘海明","id":"af02ac33-8631-4966-b331-591677e51589","originalAuthorName":"刘海明"}],"doi":"10.3969/j.issn.1004-244X.2003.02.008","fpage":"30","id":"44ecefe7-58f8-4461-906e-467ae7c16691","issue":"2","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":"f14fd4b0-e543-4ec4-85da-141af127f4a1","keyword":"晶界","originalKeyword":"晶界"},{"id":"ab14c434-8b2d-4e18-a0b0-707b42c02d72","keyword":"电容","originalKeyword":"电容"},{"id":"f2ec233c-c011-47ff-8c4f-e5218b56788e","keyword":"失真度","originalKeyword":"失真度"},{"id":"81833432-2781-48b4-8cce-dbf7ad3a56a4","keyword":"电阻率","originalKeyword":"电阻率"}],"language":"zh","publisherId":"bqclkxygc200302008","title":"晶界对信号<span style=\"color:red\">传输</span>的电容效应研究","volume":"26","year":"2003"},{"abstractinfo":"基于透镜扩束系统,应用棱镜耦合技术对液晶层的全漏导模特性进行了研究.采用盒厚为4.6 μm的<span style=\"color:red\">平行</span>排列向列相液晶盒,其内灌注E7液晶,通过实验给出了<span style=\"color:red\">平行</span>排列向列相液晶薄层的导波图,进而将实验结果与理论模拟结果进行了比较,理论所预言的液晶波导的导模在实验的导波图上得到了很好的验证.","authors":[{"authorName":"李志广","id":"a4bcdf6f-e05d-4974-b904-88db7a13afb1","originalAuthorName":"李志广"},{"authorName":"叶文江","id":"b94ec05e-0216-4910-a104-3c5eb2e76306","originalAuthorName":"叶文江"},{"authorName":"郭婷婷","id":"a1c0f3f8-28f7-4f15-8d53-e179a185c79d","originalAuthorName":"郭婷婷"},{"authorName":"张志东","id":"45c3ef92-8398-486e-b957-a66d06334442","originalAuthorName":"张志东"},{"authorName":"檀润华","id":"3fad2230-29ba-4078-934b-f8eacdf0a36d","originalAuthorName":"檀润华"}],"doi":"10.3969/j.issn.1007-2780.2009.06.009","fpage":"818","id":"3742a0da-db02-4105-ab36-3aaf0cf15546","issue":"6","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示   "},"keywords":[{"id":"0f48ed83-2eed-4b3c-bf8b-e33ba3eb1806","keyword":"向列相液晶","originalKeyword":"向列相液晶"},{"id":"c572b933-0f29-4fb3-a22a-42651fb3bba6","keyword":"透镜扩束系统","originalKeyword":"透镜扩束系统"},{"id":"82333305-e8ba-432a-a31d-07d75796a1f3","keyword":"导波","originalKeyword":"导波"},{"id":"be54e218-c0b2-4618-b408-330f1d4567ef","keyword":"导模","originalKeyword":"导模"},{"id":"d9a0a513-d320-4f59-9cac-0ea6ed6a9b1e","keyword":"波导","originalKeyword":"波导"}],"language":"zh","publisherId":"yjyxs200906009","title":"<span style=\"color:red\">平行</span>排列向列相液晶的导波研究","volume":"24","year":"2009"},{"abstractinfo":"介绍了软X射线光栅分束镜Mach-Zehnder干涉等离子体诊断系统调整用双频光栅线条<span style=\"color:red\">平行</span>度的衍射法测量系统.该系统主要由激光器,<span style=\"color:red\">准</span>直镜,待测光栅,精密转台(含角度测量仪),直线工作台,光栅调节架和探测器组成.分析了系统中各种误差对测量精度的影响其中包括距离测量误差、波长误差、光栅<span style=\"color:red\">准</span>直误差即光栅刻线与入射光和反射光组成的平面不垂直、光栅转动过程的误差、光栅表面面型误差、探测器误差,经计算得到系统的绝对误差为minute.计算表明,该系统的测量精度满足软X射线Mach-Zehnder干涉系统对双频调整光栅的性能要求.","authors":[{"authorName":"谭鑫","id":"703e9432-3126-4196-9c47-80d8eea24cba","originalAuthorName":"谭鑫"},{"authorName":"刘颖","id":"f68a8d70-b458-4e5b-92aa-013e076c447d","originalAuthorName":"刘颖"},{"authorName":"刘正坤","id":"49aa5511-5bfb-4dcc-9884-7dacc28d1241","originalAuthorName":"刘正坤"},{"authorName":"付绍军","id":"1eac01be-05bf-440e-b3d4-f1b3356b33c9","originalAuthorName":"付绍军"}],"doi":"10.3969/j.issn.1007-4252.2009.01.010","fpage":"61","id":"10761cd4-c707-4cb7-a0a0-0bdfbfe0e1f3","issue":"1","journal":{"abbrevTitle":"GNCLYQJXB","coverImgSrc":"journal/img/cover/GNCLYQJXB.jpg","id":"34","issnPpub":"1007-4252","publisherId":"GNCLYQJXB","title":"功能材料与器件学报   "},"keywords":[{"id":"694e862e-f1f5-4e37-8131-a5cf3464bf8e","keyword":"双频光栅","originalKeyword":"双频光栅"},{"id":"0eb5641f-56b4-4e3e-b826-73746a8c2d45","keyword":"<span style=\"color:red\">平行</span>度","originalKeyword":"平行度"},{"id":"d2d19637-cd24-4e8e-90e5-6d389cd2272c","keyword":"衍射法","originalKeyword":"衍射法"}],"language":"zh","publisherId":"gnclyqjxb200901010","title":"衍射法X射线激光分束光栅<span style=\"color:red\">平行</span>度测量系统","volume":"15","year":"2009"},{"abstractinfo":"当光通过一个光学器件时,一种减少两通光面反射损耗的方法,是将此两通光面切割成所谓的布儒斯特角且相互<span style=\"color:red\">平行</span>.这种相互<span style=\"color:red\">平行</span>的具有布儒斯特角通光面的光学器件,被用来减少反射损耗已经很多年了.激光发明以后,特别是二次谐波发生实现以后,上述这种<span style=\"color:red\">平行</span>式布儒斯特角切割方法,也曾不断用来降低倍频器的反射损失.但并没有人谈到过实验结果:这种将倍频器的通光面切割成相互<span style=\"color:red\">平行</span>的具有布儒斯特角的方法,是否真能减少倍频器的反射损耗?我们的回答是:不能.本文将从理论上说明为什么不能,并给出我们认为正确的切割方法.","authors":[{"authorName":"沈德忠","id":"c9329f75-9ebf-41f4-96be-53a810ff919c","originalAuthorName":"沈德忠"},{"authorName":"沈光球","id":"aa9af885-b741-4cc8-b776-85210b428642","originalAuthorName":"沈光球"},{"authorName":"王晓青","id":"adf5a436-6a81-446b-b413-4a3c34381f91","originalAuthorName":"王晓青"},{"authorName":"王晓洋","id":"d32b5867-643e-478f-bd68-26e5e3ce9128","originalAuthorName":"王晓洋"},{"authorName":"李卫","id":"0a963363-8a67-424a-9c5b-9de3d2b77efb","originalAuthorName":"李卫"},{"authorName":"王胜军","id":"bd8b168d-316c-4e26-a475-7db942370299","originalAuthorName":"王胜军"},{"authorName":"袁欣","id":"e7617896-dfa2-4ee9-8088-19f816e0d1ec","originalAuthorName":"袁欣"},{"authorName":"齐家宝","id":"432b9ec9-bee8-44d3-8f6e-338e450a6ef1","originalAuthorName":"齐家宝"}],"doi":"10.3969/j.issn.1000-985X.2000.02.001","fpage":"95","id":"f91f8517-bb62-4800-a628-d52193eae308","issue":"2","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":"e6d0f5f2-3aaf-4b8e-9f39-1fb99ad21b21","keyword":"布儒斯特角","originalKeyword":"布儒斯特角"},{"id":"1cb12c57-9d14-4c21-a088-1239deafdf9f","keyword":"激光变频器","originalKeyword":"激光变频器"},{"id":"ad865f36-a2ff-45d6-ab9b-b0ba20041683","keyword":"非<span style=\"color:red\">平行</span>通光面","originalKeyword":"非平行通光面"},{"id":"3a0187b5-6ad8-43fe-8be4-75727b59fd33","keyword":"非线性光学器件","originalKeyword":"非线性光学器件"}],"language":"zh","publisherId":"rgjtxb98200002001","title":"非<span style=\"color:red\">平行</span>通光面激光变频器","volume":"29","year":"2000"},{"abstractinfo":"对放置于手征介质中的两根<span style=\"color:red\">平行</span>手征光纤之间的耦合系数 进行了详细的数值计算和讨论，给出了耦合系数随手征参数、相对介 电常数、归一化频率、光纤之间的距离等的变化关系曲线。","authors":[{"authorName":"董建峰","id":"3f1b6728-9b39-4e02-bb38-ad927c1ab36f","originalAuthorName":"董建峰"},{"authorName":"陶卫东","id":"a7c8569d-1e86-478c-9e59-9b46b5344726","originalAuthorName":"陶卫东"}],"doi":"10.3969/j.issn.1007-5461.2000.01.003","fpage":"11","id":"3f97a08c-621d-4546-8bec-c8a568d34c2f","issue":"1","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":"c03d08f5-3bee-482e-9783-80c40094a53d","keyword":"手征参数","originalKeyword":"手征参数"},{"id":"0a7c85bc-68b2-43ab-aadf-7c7e16d721b1","keyword":"手征光纤","originalKeyword":"手征光纤"},{"id":"0b3827f2-ce2c-4773-9ab8-e0b732462a92","keyword":"耦合系数","originalKeyword":"耦合系数"}],"language":"zh","publisherId":"lzdzxb200001003","title":"<span style=\"color:red\">平行</span>手征光纤之间的耦合系数","volume":"17","year":"2000"}],"totalpage":498,"totalrecord":4975}