{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"用手征<span style=\"color:red\">SU</span>(<span style=\"color:red\">3</span>)夸克模型分析了(0s)6组态的六夸克态能量，结果表明手征<span style=\"color:red\">SU</span>(<span style=\"color:red\">3</span>)介子场可以对某些多奇异数的态提供较强的吸引作用．进一步用共振群方法研究了(ΩΩ)0+及(Ω )1+等多奇异数系统，得到(ΩΩ)0是一个深度束缚的双重态．","authors":[{"authorName":"张宗烨","id":"1b0a8a45-e2a4-4de6-ae65-6c630e098750","originalAuthorName":"张宗烨"},{"authorName":"余友文","id":"8f91a450-5e78-46e2-9e2f-963e02ccb112","originalAuthorName":"余友文"},{"authorName":"袁秀青","id":"9ce5141d-fb71-435c-8327-1621d08a3b4e","originalAuthorName":"袁秀青"}],"doi":"10.3969/j.issn.1007-4627.2000.01.003","fpage":"6","id":"e4bb15fd-81e3-4d1c-aebf-5de169720dc2","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":"fcf3cc99-3d74-43d7-9369-8a8a5981aa1b","keyword":"夸克模型","originalKeyword":"夸克模型"},{"id":"92e6e07d-8f86-462c-a66d-0dff9238277b","keyword":"六夸克态","originalKeyword":"六夸克态"},{"id":"6f454721-3a0c-4419-a307-f221acd9fe46","keyword":"手征对称性","originalKeyword":"手征对称性"}],"language":"zh","publisherId":"yzhwlpl200001003","title":"手征<span style=\"color:red\">SU</span>(<span style=\"color:red\">3</span>)夸克模型与六夸克态的研究","volume":"17","year":"2000"},{"abstractinfo":"建立了SO(8)同位旋标量、同位旋矢量及总的配对基与微观壳模型坐标空间部分的Elliott <span style=\"color:red\">SU</span>(<span style=\"color:red\">3</span>)基之间的对应关系.从该代数间的互补关系导出了在壳模型的粒子数守恒代数U(4Ω)中所包含的具有同位旋T及自旋S的Wigner超多重态(不可约)表示.其重要性在于,该结果能用于研究对相互作用和四极-四极相互作用在核谱中的竞争效应并揭示其配对基中的<span style=\"color:red\">SU</span>(<span style=\"color:red\">3</span>)组份.虽然仅展示了该理论对ds壳的计算,其方法也适用于研究多壳的情形.","authors":[{"authorName":"Ana Ivanova Georgieva","id":"c5de90c1-04e6-47a6-93dd-07e8d8021f62","originalAuthorName":"Ana Ivanova Georgieva"},{"authorName":"Kalin Pavlov Drumev","id":"5c386d84-e4b0-4e18-a9b1-f1469001fab4","originalAuthorName":"Kalin Pavlov Drumev"}],"doi":"10.11804/NuclPhysRev.34.01.062","fpage":"62","id":"5be20482-f43d-421f-9b59-fc03461998f8","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":"87c872ab-2e1c-46d2-8c09-04a2a1a1cbc7","keyword":"代数模型","originalKeyword":"代数模型"},{"id":"8939b3b1-8c38-4619-a160-a0aeca9105d1","keyword":"对相互作用","originalKeyword":"对相互作用"},{"id":"561f3a24-5ad2-4fe0-8b51-a73a4464345b","keyword":"四极-四极相互作用","originalKeyword":"四极-四极相互作用"},{"id":"03fab655-a063-4652-b814-c5082b63ea87","keyword":"壳模型","originalKeyword":"壳模型"},{"id":"a9a05f51-8b49-47bb-8373-d45e1a58c043","keyword":"自旋-同位旋空间","originalKeyword":"自旋-同位旋空间"}],"language":"zh","publisherId":"yzhwlpl201701013","title":"SO(8)对关联和代数壳模型中的<span style=\"color:red\">SU</span>(<span style=\"color:red\">3</span>)四极基底","volume":"34","year":"2017"},{"abstractinfo":"γ射线能量自旋曲线指认156Gd核基态具有<span style=\"color:red\">SU</span>(<span style=\"color:red\">3</span>)和O(6)两种对称性.基于微观sdIBM-(F)max方案和单粒子能量实验值,用两组核子之间的对作用、四极对作用、四极-四极作用的等效强度参数,都很好地再现了这两种能谱及其演化过程.计算结果揭示出对基态相变的一种新理解:<span style=\"color:red\">SU</span>(<span style=\"color:red\">3</span>)的基准态是低激发-低有序态,而O(6)基准态则是高激发-高有序的,它们有临界区6+1-8+1态;当核退耦到临界区时,高有序基准态释放多余的有序结构能,导致低有序基准态重组,实现减速旋转驱动高有序核向着低有序核过渡的量子相变.最后用156Gd核的势能曲面作了直观说明.","authors":[{"authorName":"雷玉玺","id":"6c930305-ac1e-47cd-b5dd-9c2619d7dfef","originalAuthorName":"雷玉玺"},{"authorName":"张欢","id":"487b8cb5-81e9-4624-995b-848f9cff759d","originalAuthorName":"张欢"},{"authorName":"石筑一","id":"f359a543-a119-413c-bcdb-376fa2cf5a99","originalAuthorName":"石筑一"},{"authorName":"汪红","id":"51f6289b-ee8c-455b-a329-609f430990bb","originalAuthorName":"汪红"},{"authorName":"童红","id":"bcbcb2c5-0eb8-4358-a59d-c7e090bc0e90","originalAuthorName":"童红"}],"doi":"","fpage":"257","id":"941a12a5-4b77-43bb-a800-6bba27208747","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":"7eca6bf9-0bc6-4d47-aeb8-8e0eda97fbec","keyword":"量子相变","originalKeyword":"量子相变"},{"id":"5d7a6c0b-54b3-45b1-a19c-1393d1f5f635","keyword":"基态结构演化","originalKeyword":"基态结构演化"},{"id":"ca8e5d91-9d14-40f3-a5bd-ce8c720ee03c","keyword":"微观sdIBM-(F)max方案","originalKeyword":"微观sdIBM-(F)max方案"},{"id":"ca77d961-771f-454f-b5b2-48cadf6c4ccf","keyword":"156Gd核","originalKeyword":"156Gd核"}],"language":"zh","publisherId":"yzhwlpl201003003","title":"156Gd基态<span style=\"color:red\">SU</span>(<span style=\"color:red\">3</span>)→O(6)相变的一种微观理解","volume":"27","year":"2010"},{"abstractinfo":"介绍了多夸克态研究的重要性, 侧重介绍了最近发现的5夸克态的实验和理论研究现况.","authors":[{"authorName":"张宗烨","id":"35ef1c88-b3f3-4a06-9851-95ccad58f00e","originalAuthorName":"张宗烨"}],"doi":"10.3969/j.issn.1007-4627.2004.04.001","fpage":"263","id":"1f7a9495-8f94-460b-8693-f444c4be03fc","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":"42ecbd58-9e7d-4b03-aa3a-9ad5e59e7fd2","keyword":"五夸克态","originalKeyword":"五夸克态"},{"id":"bb779de4-21bb-49fe-b3ea-f6f56729d440","keyword":"夸克模型","originalKeyword":"夸克模型"},{"id":"9d5cd511-a3aa-4058-86f8-72e4a26a0d80","keyword":"<span style=\"color:red\">SU</span>(<span style=\"color:red\">3</span>)","originalKeyword":"SU(3)"}],"language":"zh","publisherId":"yzhwlpl200404001","title":"多夸克态研究概况","volume":"21","year":"2004"},{"abstractinfo":"","authors":[{"authorName":"R.L.Kelly","id":"da237e66-719c-46c7-95f7-a97c51623e2f","originalAuthorName":"R.L.Kelly"}],"doi":"","fpage":"506","id":"8e496b30-e10d-426b-ace9-64c3f06ce8c9","issue":"9","journal":{"abbrevTitle":"ZGWLC","coverImgSrc":"journal/img/cover/ZGWLC.jpg","id":"85","issnPpub":"1674-1137","publisherId":"ZGWLC","title":"中国物理C"},"keywords":[{"id":"82acebb8-ffee-47c1-980e-b1211487f5c5","keyword":"","originalKeyword":""}],"language":"zh","publisherId":"zgwl-c201409046","title":"<span style=\"color:red\">SU</span>(<span style=\"color:red\">3</span>) ISOSCALAR FACTORS AND REPRESENTATION MATRICES","volume":"38","year":"2014"},{"abstractinfo":"通过改变<span style=\"color:red\">SU</span>-8光刻胶中PAG浓度获得含不同PAG浓度的各种改性<span style=\"color:red\">SU</span>-8光刻胶,在对其光学性能以及最小曝光剂量的测定基础上研究改性<span style=\"color:red\">SU</span>-8光刻胶的光刻工艺,借助于改性<span style=\"color:red\">SU</span>-8光刻胶的合理设计以及背面曝光和正面曝光的结合应用提高多元材料复杂结构的集成制造能力.","authors":[{"authorName":"朱军","id":"ec770568-32ba-47ec-acd6-2c5498b1e9fc","originalAuthorName":"朱军"},{"authorName":"蒋宏民","id":"48193798-8acd-4273-965f-98e648b4027f","originalAuthorName":"蒋宏民"},{"authorName":"陈翔","id":"dacdbf85-dfa3-4118-ad5a-a005173ebbee","originalAuthorName":"陈翔"},{"authorName":"陈迪","id":"45ce2355-72a6-4453-8168-2e319df26c8c","originalAuthorName":"陈迪"},{"authorName":"刘景全","id":"9317fde9-8900-47ef-85a2-57a0c638868f","originalAuthorName":"刘景全"}],"doi":"10.3969/j.issn.1007-4252.2009.03.009","fpage":"259","id":"dcd046b2-7c6b-44a5-b7ee-3a44371e0f03","issue":"3","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":"54c24b04-877d-446d-9f03-be15c55e1e31","keyword":"最小曝光剂量","originalKeyword":"最小曝光剂量"},{"id":"ab34b1c2-47da-4d9a-a6e0-5dba289535f0","keyword":"PAG","originalKeyword":"PAG"},{"id":"40c5ad50-b6ce-428c-8128-fdf6b84db493","keyword":"集成制造","originalKeyword":"集成制造"}],"language":"zh","publisherId":"gnclyqjxb200903009","title":"改性<span style=\"color:red\">SU</span>8光刻胶的光学特性及其工艺","volume":"15","year":"2009"},{"abstractinfo":"PDMS是制作微流控芯片的主要材料.PDMS芯片制作的主要方法是模塑法,模塑法要求有良好的塑性成型模具.<span style=\"color:red\">SU</span>-8以其良好的微加工特性,目前已广泛应用于微机械结构的制作,也用于PDMS塑性成型的模具.本文根据模具的特殊性,如平整、无裂纹、可多次使用等要求,研究了影响<span style=\"color:red\">SU</span>-8模具结构与基底材料硅片的黏附性和形成裂纹的因素,优化了<span style=\"color:red\">SU</span>-8微模具加工工艺,在以0.5℃/min进行升降温、210 mJ/cm2的曝光剂量、200℃条件下硬烘30min条件下得到较好的<span style=\"color:red\">SU</span>-8模具,提供了一种快速、复用性高、低成本的PDMS微芯片塑性成型的<span style=\"color:red\">SU</span>-8模具的制作方法.","authors":[{"authorName":"陆振华","id":"8c2123aa-3ba7-438c-ab5a-a64d00fb1c75","originalAuthorName":"陆振华"},{"authorName":"许宝建","id":"cd73f0d1-93c5-441a-b43d-27cdbfa9ca4d","originalAuthorName":"许宝建"},{"authorName":"金庆辉","id":"d5ba9278-8fc9-40f3-8436-9dae3ee0ac5b","originalAuthorName":"金庆辉"},{"authorName":"赵建龙","id":"6ac47d32-7041-4960-8a1c-d2eafabd5eae","originalAuthorName":"赵建龙"}],"doi":"10.3969/j.issn.1007-4252.2008.03.015","fpage":"639","id":"3020bfc4-b6ae-4ae2-ad16-b3fa3c778870","issue":"3","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":"d3418548-8b1e-4f1f-baa3-28ac1362f03d","keyword":"PDMS","originalKeyword":"PDMS"},{"id":"68402aea-2b68-4a8a-83ea-71fd695cc2ef","keyword":"塑性成型","originalKeyword":"塑性成型"},{"id":"36b99e1d-6110-4e46-8e64-083ba672b590","keyword":"<span style=\"color:red\">SU</span>-8模具","originalKeyword":"SU-8模具"},{"id":"852ecbaf-7a7e-410e-94c1-57f55129c452","keyword":"黏附性","originalKeyword":"黏附性"}],"language":"zh","publisherId":"gnclyqjxb200803015","title":"用于PDMS微芯片塑性成型的<span style=\"color:red\">SU</span>-8模具制作工艺的优化","volume":"14","year":"2008"},{"abstractinfo":"利用静电纺丝和紫外光刻技术直接制备了不同结构的<span style=\"color:red\">SU</span>-8光刻胶纳米纤维薄膜及图案阵列.通过光学显微镜和扫描电子显微镜表征了纳米纤维的形貌、尺寸及结构.结果表明,通过改变<span style=\"color:red\">SU</span>-8光刻胶的黏度可形成不同直径和形貌的纤维结构,其中用<span style=\"color:red\">SU</span>-8 3010和<span style=\"color:red\">SU</span>-8 3050光刻胶制备的纳米纤维具有最优的形貌,其平均直径分别为470 nm和610nm.利用带有长方形缺口的铝箔和同轴电纺的方法分别制备了平行趋向和空心结构的纳米纤维.通过紫外光刻过程,可将<span style=\"color:red\">SU</span>-8纳米纤维加工成点阵、条状等不同形貌的图案阵列或结构,有望用作细胞培养研究的功能基底材料.","authors":[{"authorName":"刘俊","id":"9b7b51f7-f00d-40d6-b12a-9992f70bebdf","originalAuthorName":"刘俊"},{"authorName":"常梦洁","id":"e235ab1f-9c42-4c68-8f3d-e87c5d1c2435","originalAuthorName":"常梦洁"},{"authorName":"杜慧玲","id":"d9dbc0f1-d81a-4b33-81f8-942a5df5af80","originalAuthorName":"杜慧玲"}],"doi":"10.16865/j.cnki.1000-7555.2016.04.023","fpage":"121","id":"709a57e8-a39b-4a45-9373-191bade8c9ba","issue":"4","journal":{"abbrevTitle":"GFZCLKXYGC","coverImgSrc":"journal/img/cover/GFZCLKXYGC.jpg","id":"31","issnPpub":"1000-7555","publisherId":"GFZCLKXYGC","title":"高分子材料科学与工程"},"keywords":[{"id":"5d7322d3-bbd6-489b-b6da-aafd8926cbc1","keyword":"静电纺丝","originalKeyword":"静电纺丝"},{"id":"49545022-d435-4dba-9058-8ee5a48f03f2","keyword":"纳米纤维","originalKeyword":"纳米纤维"},{"id":"3c6f3c34-5ec1-4746-91ab-634bb7d72a9f","keyword":"<span style=\"color:red\">SU</span>-8光刻胶","originalKeyword":"SU-8光刻胶"},{"id":"4c0080ec-38e0-4d4a-9070-a8a325161206","keyword":"纤维图案","originalKeyword":"纤维图案"}],"language":"zh","publisherId":"gfzclkxygc201604023","title":"静电纺丝制备<span style=\"color:red\">SU</span>-8光刻胶纳米纤维及图案阵列","volume":"32","year":"2016"},{"abstractinfo":"采用新型<span style=\"color:red\">SU</span>-8光刻胶在UV-LIGA技术基础上制备了各种高深宽比MEMS微结构,研究了热处理和曝光两个重要因素对高深宽比微结构的影响,解决了微结构的开裂和倒塌等问题;优化了<span style=\"color:red\">SU</span>-8胶工艺,从而获得了最大深宽比为27:1的微结构.","authors":[{"authorName":"张金娅","id":"0601906a-f263-4410-92c1-2687a433f1cc","originalAuthorName":"张金娅"},{"authorName":"陈迪","id":"686bf8a4-0539-47db-bcd5-73b442b6fb8c","originalAuthorName":"陈迪"},{"authorName":"朱军","id":"c38a5769-bd5b-43b0-96c5-2414216cc362","originalAuthorName":"朱军"},{"authorName":"李建华","id":"454f5c90-82f2-4a97-bca7-81a602404205","originalAuthorName":"李建华"},{"authorName":"方华斌","id":"32d4de2f-02ee-41dc-9c3f-1a0ae396576f","originalAuthorName":"方华斌"},{"authorName":"杨斌","id":"0b516beb-a962-423f-98b5-69c12d942b9f","originalAuthorName":"杨斌"}],"doi":"10.3969/j.issn.1007-4252.2005.02.027","fpage":"251","id":"a60d85a7-1d30-45f4-afcc-ea8e848e6cbe","issue":"2","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":"d7a3b40d-2930-44f1-a47c-2e80fa1d7bc1","keyword":"UV-LIGA技术","originalKeyword":"UV-LIGA技术"},{"id":"84414101-485a-483f-9e57-def5743e93c2","keyword":"<span style=\"color:red\">SU</span>-8胶","originalKeyword":"SU-8胶"},{"id":"86816471-713e-4968-a03d-1a50ebb253e7","keyword":"高深宽比微结构","originalKeyword":"高深宽比微结构"}],"language":"zh","publisherId":"gnclyqjxb200502027","title":"超厚<span style=\"color:red\">SU</span>-8负胶高深宽比结构及工艺研究","volume":"11","year":"2005"},{"abstractinfo":"构造了激发双模<span style=\"color:red\">SU</span>(2)相干态|M,ξ;m〉=AMξma+mb+m|M,ξ〉,并用数值方法研究其非经典特性.结果表明,在双模<span style=\"color:red\">SU</span>(2)相干态的两场模同时增加光子后,两模光场仍然保持反关联特性,而且可以使光场对Cauchy-Schwartz不等式的破坏程度、光场的反聚束效应以及光子统计亚泊松分布等非经典特性得到加强.","authors":[{"authorName":"黄纯青","id":"f334aa8d-452d-4bdf-9c36-4956ef67713d","originalAuthorName":"黄纯青"},{"authorName":"万广仁","id":"5f4134f1-549f-4603-9ef2-86a4b3433879","originalAuthorName":"万广仁"}],"doi":"10.3969/j.issn.1007-5461.2005.01.009","fpage":"47","id":"a0d78717-a00e-4e4d-8d07-cac79b31fe98","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":"a09ea400-1246-4a1a-a2e0-a5307f3ea02e","keyword":"量子光学","originalKeyword":"量子光学"},{"id":"0da7bb42-1903-4b57-8a98-6715060b4f77","keyword":"非经典特性","originalKeyword":"非经典特性"},{"id":"cff04856-ac58-43f4-8287-b477c266bdc0","keyword":"激发","originalKeyword":"激发"},{"id":"ddf1087d-484e-4619-998c-b4478ddcb995","keyword":"双模<span style=\"color:red\">SU</span>(2)相干态","originalKeyword":"双模SU(2)相干态"}],"language":"zh","publisherId":"lzdzxb200501009","title":"激发双模<span style=\"color:red\">SU</span>(2)相干态的非经典性质","volume":"22","year":"2005"}],"totalpage":6219,"totalrecord":62189}