{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"简要介绍了Skyrme模型及其对重子的描述,给出了3个不同于Balachandran解的双重子<span style=\"color:red\">手</span><span style=\"color:red\">征</span><span style=\"color:red\">孤子</span>解,并用Witten的方法量子化这些<span style=\"color:red\">孤子</span>,得出双重子<span style=\"color:red\">手</span><span style=\"color:red\">征</span><span style=\"color:red\">孤子</span>质量谱,这些<span style=\"color:red\">孤子</span>的空间对称性质不同,有相同的质量谱.","authors":[{"authorName":"周小方","id":"41e111d9-621d-47d4-8f0b-c0b67fa2794b","originalAuthorName":"周小方"}],"doi":"10.3969/j.issn.1007-4627.2007.01.002","fpage":"6","id":"3a43b499-5ca4-48bc-8cf1-d20cc8ed8ac3","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   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style=\"color:red\">手</span><span style=\"color:red\">征</span>角，发现经过第一次迭代后，指数形式的<span style=\"color:red\">手</span><span style=\"color:red\">征</span>角给出的结果比别的<span style=\"color:red\">手</span><span style=\"color:red\">征</span>角更接近自洽解的形状。","authors":[{"authorName":"江学敏","id":"3cf004b2-c579-4ed1-8579-c6cb888aa6a0","originalAuthorName":"江学敏"},{"authorName":"李云德","id":"8aeed121-4bc1-44dd-95b6-30744a920145","originalAuthorName":"李云德"}],"doi":"10.11804/NuclPhysRev.32.04.405","fpage":"405","id":"05ead77f-e4ed-4cba-830b-0d8b60c6003d","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":"5bf10afd-1502-4e03-bbd2-6c6bc4ded8f8","keyword":"自洽<span style=\"color:red\">孤子</span>解","originalKeyword":"自洽孤子解"},{"id":"7df04aa3-7a1b-48c1-b314-a35751ee0c0d","keyword":"<span style=\"color:red\">手</span><span style=\"color:red\">征</span>夸克<span 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style=\"color:red\">征</span>方法实现负折射的特点和优势,展现了该方法的潜在应用前景.","authors":[{"authorName":"董建峰","id":"4c6a2128-127e-44cb-85a5-affcbcc002b2","originalAuthorName":"董建峰"},{"authorName":"徐超","id":"6d8c26dd-68a6-477a-ba48-fc79b0224cf8","originalAuthorName":"徐超"},{"authorName":"徐键","id":"b7b45f73-e984-48ac-bc66-5277dae9fa35","originalAuthorName":"徐键"}],"doi":"10.3969/j.issn.1007-5461.2009.04.001","fpage":"385","id":"35148516-04f3-40aa-aa8a-c765a349afff","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":"d3ae14e3-e1cf-4f07-871e-d89420f14ed5","keyword":"光电子学","originalKeyword":"光电子学"},{"id":"4c6ce14e-45e6-466a-bb49-7b34ac2f51de","keyword":"负折射","originalKeyword":"负折射"},{"id":"4c89d718-2f38-46cc-b5cd-4f5e9c3862c6","keyword":"<span style=\"color:red\">手</span><span style=\"color:red\">征</span>性","originalKeyword":"手征性"},{"id":"2a96d881-c8ca-47cc-853c-cdd6e2acdd86","keyword":"完美透镜","originalKeyword":"完美透镜"},{"id":"f22fe2a8-30ec-4fe0-b456-3ff62917727a","keyword":"旋光性","originalKeyword":"旋光性"}],"language":"zh","publisherId":"lzdzxb200904001","title":"<span style=\"color:red\">手</span><span style=\"color:red\">征</span>负折射研究进展","volume":"26","year":"2009"},{"abstractinfo":"<span style=\"color:red\">手</span><span style=\"color:red\">征</span>微扰论是基于量子色动力学的低能有效理论, 已成为核物理和低能粒子物理研究的有力方法. 简单介绍了<span style=\"color:red\">手</span><span style=\"color:red\">征</span>微扰论的基本概念、方法和应用, 特别是近年来重子<span style=\"color:red\">手</span><span style=\"color:red\">征</span>微扰论的形式发展和一些应用中的前沿问题. ","authors":[{"authorName":"张小兵","id":"b9f94d3d-7e01-488e-aa96-fbeeeef5596f","originalAuthorName":"张小兵"},{"authorName":"李磊","id":"771317b1-dab0-4981-bc8a-8f5a0adf28a3","originalAuthorName":"李磊"},{"authorName":"宁平治","id":"3d2fa7d4-0b73-4305-8839-efec05df056c","originalAuthorName":"宁平治"}],"doi":"10.3969/j.issn.1007-4627.2002.01.005","fpage":"24","id":"caa0fee1-3c3d-427f-8d27-3a67235a5e39","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":"f0db7c99-935a-414a-b135-eae8ca62c4bc","keyword":"<span style=\"color:red\">手</span><span style=\"color:red\">征</span>微扰论","originalKeyword":"手征微扰论"},{"id":"f846e835-2157-4d2c-a910-72b79e8d6684","keyword":"<span style=\"color:red\">手</span><span style=\"color:red\">征</span>对称性","originalKeyword":"手征对称性"},{"id":"7db9573a-30c0-45ee-a09d-956eb72c36da","keyword":"有效场论","originalKeyword":"有效场论"}],"language":"zh","publisherId":"yzhwlpl200201005","title":"核物理中的<span style=\"color:red\">手</span><span style=\"color:red\">征</span>微扰论","volume":"19","year":"2002"},{"abstractinfo":"对放置于<span style=\"color:red\">手</span><span style=\"color:red\">征</span>介质中的两根平行<span style=\"color:red\">手</span><span style=\"color:red\">征</span>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<span style=\"color:red\">手</span><span style=\"color:red\">征</span>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":"<span style=\"color:red\">手</span><span style=\"color:red\">征</span>参数","originalKeyword":"手征参数"},{"id":"0a7c85bc-68b2-43ab-aadf-7c7e16d721b1","keyword":"<span style=\"color:red\">手</span><span style=\"color:red\">征</span>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":"平行<span style=\"color:red\">手</span><span style=\"color:red\">征</span>光纤之间的耦合系数","volume":"17","year":"2000"},{"abstractinfo":"在对双包层<span style=\"color:red\">手</span><span style=\"color:red\">征</span>光纤(W型)进行解析求解的基础上,用数值计算方法研究了纤芯和内外包层的<span style=\"color:red\">手</span><span style=\"color:red\">征</span>参数和内包层厚度对模式色散特性的影响,给出了双包层<span style=\"color:red\">手</span><span style=\"color:red\">征</span>光纤中基模的归一化传播常数b、群延迟d(Vb)/dV和波导色散Vd2(Vb)/dV2随纤芯和内外包层的<span style=\"color:red\">手</span><span style=\"color:red\">征</span>参数和内包层厚度的变化关系曲线,结果表明在双包层光纤的纤芯和内外包层中引入<span style=\"color:red\">手</span><span style=\"color:red\">征</span>,可以极大地改变光纤中基模的色散特性,特别是内包层厚度不同时,色散特性也极为不同.","authors":[{"authorName":"董建峰","id":"903a3237-a082-4a96-950d-7304a9b27d14","originalAuthorName":"董建峰"},{"authorName":"陶卫东","id":"4106f07b-2eac-4360-984b-d791484d157a","originalAuthorName":"陶卫东"},{"authorName":"聂秋华","id":"f06229bf-030d-445e-817a-0b35602be1f9","originalAuthorName":"聂秋华"}],"doi":"10.3969/j.issn.1007-5461.2003.04.020","fpage":"482","id":"ca23cea3-17e8-4a84-bda1-30f68f47c0c8","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":"71f9f1f8-2f08-4217-9fd7-df132e1c10da","keyword":"<span style=\"color:red\">手</span><span style=\"color:red\">征</span>光纤","originalKeyword":"手征光纤"},{"id":"c9ffdde4-bdf0-4bda-998a-ff2358da1ecc","keyword":"双包层光纤","originalKeyword":"双包层光纤"},{"id":"c20ba1a5-387d-4c5d-8776-13d8d164430c","keyword":"传播常数","originalKeyword":"传播常数"},{"id":"dbd866a3-4197-49d0-8d76-578b87a7042b","keyword":"群延迟","originalKeyword":"群延迟"},{"id":"3dca58df-55fb-49d1-89c3-50ef9d396ee9","keyword":"波导色散","originalKeyword":"波导色散"}],"language":"zh","publisherId":"lzdzxb200304020","title":"双包层<span style=\"color:red\">手</span><span style=\"color:red\">征</span>光纤的色散特性","volume":"20","year":"2003"},{"abstractinfo":"利用三轴形变的粒子-转子模型讨论了A≈100和A≈130核区<span style=\"color:red\">手</span><span style=\"color:red\">征</span>双重带. 基于粒子空穴组态πh11/2(○)νh-111/2的计算很好地再现了A≈130核区 N=75同中子素的<span style=\"color:red\">手</span><span style=\"color:red\">征</span>双重带实验能谱. 通过分析基于组态πg9/2(○)νg-19/2的约化跃迁几率B(E2)和B(M1)研究A≈100核区可能的<span style=\"color:red\">手</span><span style=\"color:red\">征</span>双重带.","authors":[{"authorName":"彭婧","id":"3aed28cf-a319-4c76-9426-edbb31eb7b8a","originalAuthorName":"彭婧"},{"authorName":"孟杰","id":"cddc027e-09b9-4217-b3b3-3bc8a52f093d","originalAuthorName":"孟杰"},{"authorName":"张双全","id":"083aa575-272c-48c9-9d9e-1718773143b5","originalAuthorName":"张双全"}],"doi":"10.3969/j.issn.1007-4627.2004.04.028","fpage":"360","id":"c90f4120-201f-4acb-b140-de52a6262364","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":"6bd0af1d-a93a-4df0-b83e-b02832b82665","keyword":"<span style=\"color:red\">手</span><span style=\"color:red\">征</span>双重带","originalKeyword":"手征双重带"},{"id":"bf846c46-5c0f-4450-87a2-57746dccdfdf","keyword":"粒子-转子模型","originalKeyword":"粒子-转子模型"},{"id":"45e80780-d940-4697-bda1-1c4b9ece3eb2","keyword":"粒子空穴组态","originalKeyword":"粒子空穴组态"},{"id":"1ec16277-e169-4855-97fe-28d8ac7c1c8d","keyword":"约化跃迁几率","originalKeyword":"约化跃迁几率"}],"language":"zh","publisherId":"yzhwlpl200404028","title":"A≈100和130核区<span style=\"color:red\">手</span><span style=\"color:red\">征</span>双重带的描述","volume":"21","year":"2004"},{"abstractinfo":"平面<span style=\"color:red\">手</span><span style=\"color:red\">征</span>超常介质(Planar chiral metamaterials, PCM)是近年迅速发展起来的能获得大旋光性进而控制光偏振的新颖介质.综述了PCM的研究进展,包括金属结构、全介质结构以及单层和双层结构等几种不同情况,这些PCM都能产生非常强的旋光性,在光子学中具有潜在的应用前景,并且有可能成为<span style=\"color:red\">手</span><span style=\"color:red\">征</span>负折射光学材料中有前途的候选者.","authors":[{"authorName":"董建峰","id":"fe727a5b-16ed-459b-a4b9-c8e2524dc552","originalAuthorName":"董建峰"},{"authorName":"徐超","id":"80e1c001-fa2c-42fd-af63-4c295131894a","originalAuthorName":"徐超"},{"authorName":"徐键","id":"ab57c4a4-134a-4c8c-9ad4-f91b9ea7f8bc","originalAuthorName":"徐键"}],"doi":"","fpage":"84","id":"fcc36d30-4c00-4ed4-a0a6-c82884446a4a","issue":"1","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"f496749e-2e34-4119-af27-3ffd063a7793","keyword":"平面<span style=\"color:red\">手</span><span style=\"color:red\">征</span>","originalKeyword":"平面手征"},{"id":"6e969191-b685-4ab0-9364-2e60167a731c","keyword":"超常介质","originalKeyword":"超常介质"},{"id":"0da71ce7-5235-480d-9748-500458e05dd9","keyword":"旋光性","originalKeyword":"旋光性"},{"id":"68d624c5-b7ec-4c52-ab65-8823c370d566","keyword":"纳米结构","originalKeyword":"纳米结构"}],"language":"zh","publisherId":"cldb200901020","title":"平面<span style=\"color:red\">手</span><span style=\"color:red\">征</span>超常介质研究进展","volume":"23","year":"2009"},{"abstractinfo":"在<span style=\"color:red\">手</span><span style=\"color:red\">征</span>夸克模型的框架下,研究了五夸克态 uudd的结构.分别考虑了 Jπ=(1/2)-和 Jπ=(1/2)+的各四个组态.结果表明对于不同的模型,不论 Jπ=(1/2)-和 Jπ=(1/2)+,T=0 的态的能量总是最低的.但是最低态的能量的理论计算值仍比Θ质量的实验值高250-300 MeV.","authors":[{"authorName":"张宗烨","id":"04d5a8af-6ade-4f52-ab31-bd896b2f1b18","originalAuthorName":"张宗烨"},{"authorName":"黄飞","id":"c05d7049-baed-4db5-b041-f9e2ced4ea27","originalAuthorName":"黄飞"},{"authorName":"余友文","id":"c768931b-2a01-48d0-8ca3-56b01d972643","originalAuthorName":"余友文"},{"authorName":"邹冰松","id":"d4346d50-3f0f-4bd0-b671-7630a675d245","originalAuthorName":"邹冰松"}],"doi":"10.3969/j.issn.1007-4627.2004.02.003","fpage":"77","id":"eea53c67-f1c8-40ca-a973-546c4adc9ff5","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":"d220ffe5-d038-4521-a910-566ccf45105d","keyword":"禁闭夸克态","originalKeyword":"禁闭夸克态"},{"id":"4187f5d3-c16e-4d5c-a529-f8ca01fd792c","keyword":"夸克模型","originalKeyword":"夸克模型"},{"id":"697cd8b7-56de-4b06-b56e-3b10461446a8","keyword":"<span style=\"color:red\">手</span><span style=\"color:red\">征</span>对称性","originalKeyword":"手征对称性"}],"language":"zh","publisherId":"yzhwlpl200402003","title":"五夸克态Θ的<span style=\"color:red\">手</span><span style=\"color:red\">征</span>夸克模型研究","volume":"21","year":"2004"},{"abstractinfo":"讨论了在LHC的Pb-Pb碰撞过程中,如果QGP SU(2)<span style=\"color:red\">手</span><span style=\"color:red\">征</span>相变出现二级相变,那么系统将会有π弦产生,并且π弦最终将衰变为π介子.于是以上效应将导致在低动量区域(p(~-)2150-400 MeV)内的π介子增强.对应于不同的冷却温度Tf=130,120,110 MeV,产生于π弦衰变的π介子的数量分别是Nt≈270,150,60.","authors":[{"authorName":"徐晓梅","id":"564573dc-e300-41b6-a61f-de67f561934a","originalAuthorName":"徐晓梅"},{"authorName":"傅永平","id":"23188e64-003c-4fd9-b680-6013f89b018f","originalAuthorName":"傅永平"},{"authorName":"李云德","id":"1c1ea9fe-2925-43ef-865c-cf46193d7b7e","originalAuthorName":"李云德"}],"doi":"","fpage":"160","id":"fc068f24-24d1-44d8-98a2-d1e17a43bdca","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":"11de1787-f0a1-440a-ad47-2b9e54da8a4c","keyword":"π弦","originalKeyword":"π弦"},{"id":"bddc3118-43f1-4e6f-afe5-cd3767344ff5","keyword":"线性σ模型","originalKeyword":"线性σ模型"},{"id":"47bb7fea-2c42-4b0c-a618-50c105fbe3f0","keyword":"<span style=\"color:red\">手</span><span style=\"color:red\">征</span>相交","originalKeyword":"手征相交"}],"language":"zh","publisherId":"yzhwlpl201002008","title":"QCD<span style=\"color:red\">手</span><span style=\"color:red\">征</span>相变中的π介子增强","volume":"27","year":"2010"}],"totalpage":1192,"totalrecord":11911}