{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"介绍了共焦点椭球构型,给出了基于该构型对<span style=\"color:red\">空间</span><span style=\"color:red\">任意</span><span style=\"color:red\">取向</span>复合材料模量的解析计算公式,并将其同Mori-Tanaka(MT)法、Ponte-Castaneda-Willis(PCW)方法以及Hashin-Shtrikman(HS)界限进行了比较.数值结果显示,基于该构型的预测处于MT法和PCW法所预测的值之间,并且与MT法所预测的值接近.此外,还对纤维不同的角度平均方法对有效性质的影响做了讨论.","authors":[{"authorName":"马寒松","id":"4fca226b-fe7e-449e-84ae-4ebdef746bc2","originalAuthorName":"马寒松"},{"authorName":"胡更开","id":"7551a95d-95fe-4d77-9928-8bb91834b776","originalAuthorName":"胡更开"}],"doi":"10.3321/j.issn:1000-3851.2003.06.018","fpage":"92","id":"3d45211a-b06d-44cd-9d37-01da4822d1e9","issue":"6","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":"3a09f8ff-a001-40d0-b7ef-b63f80b8de3e","keyword":"共焦点椭球构型","originalKeyword":"共焦点椭球构型"},{"id":"4ee4c6de-bdc6-4bb1-ba65-ffeaa55190a7","keyword":"细观力学","originalKeyword":"细观力学"},{"id":"f1475168-5060-48d6-8c75-059a482773f0","keyword":"有效模量","originalKeyword":"有效模量"},{"id":"bd426776-af78-4da5-aaf5-d15cc5ce6ec0","keyword":"<span style=\"color:red\">空间</span><span style=\"color:red\">任意</span><span style=\"color:red\">取向</span>","originalKeyword":"空间任意取向"}],"language":"zh","publisherId":"fhclxb200306018","title":"基于共焦点椭球构型的复合材料有效性质预测","volume":"20","year":"2003"},{"abstractinfo":"本文用晶体<span style=\"color:red\">空间</span><span style=\"color:red\">取向</span>分布研究了含磷深冲钢冷轧和退火织构.仔细分析了冷轧和退火板材<span style=\"color:red\">取向</span>分布函数的特征.从观察到的特征可以认为,退火织构起源于微带和过渡带生核,随后这些再结晶晶粒借吞并基体形变织构而长大.含磷深冲钢与铝镇静深冲钢的退火板材之间晶体<span style=\"color:red\">取向</span>分布有明显的区别.","authors":[{"authorName":"胡郇","id":"c56df30a-ce9c-4f43-a388-27f1b5ab1ed8","originalAuthorName":"胡郇"}],"categoryName":"|","doi":"","fpage":"121","id":"dc04fe4b-23f3-4d3c-8f37-7640be27988b","issue":"2","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[],"language":"zh","publisherId":"0412-1961_1980_2_7","title":"含磷深冲钢冷轧和退火板材的晶体<span style=\"color:red\">空间</span><span style=\"color:red\">取向</span>分布","volume":"16","year":"1980"},{"abstractinfo":"用晶体<span style=\"color:red\">取向</span>分布函数研究了含0.13％Cu的低碳镇静钢冷轧薄板再结晶退火过程织构的变化。结果表明,冷轧织构主要为平行于板面法线的<111>纤维织构组分和{001} <110>组分;此两组分的漫散构成平行于轧向的<110>部分纤维织构。在再结晶过程中<111>纤维织构增强,{001} <110>组分减弱,因而<110>部分纤维织构也逐渐收缩,表明它不是一个独立的织构组分。","authors":[{"authorName":"黄清珠","id":"c5506235-49b1-4966-917c-8ea90aa6a308","originalAuthorName":"黄清珠"},{"authorName":"孔冰玉","id":"6729007d-fbf2-47ef-a4ab-08d038d8c0f0","originalAuthorName":"孔冰玉"},{"authorName":"祝聪训","id":"e91ed54f-8582-42d8-b52b-37702d76725e","originalAuthorName":"祝聪训"}],"categoryName":"|","doi":"","fpage":"86","id":"0d71ca03-975f-4fb6-9f64-4ba84e3aa998","issue":"6","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[],"language":"zh","publisherId":"0412-1961_1983_6_5","title":"铝镇静钢冷轧薄板再结晶退火过程的晶体<span style=\"color:red\">空间</span><span style=\"color:red\">取向</span>分布","volume":"19","year":"1983"},{"abstractinfo":"量子博弈是量子信息学最近兴起的又一分支.杜江峰等在研究连续变量量子博弈中,利用了双模压缩态实现量子纠缠并产生优于经典的结果.我们在此基础上对于有<span style=\"color:red\">任意</span>多个参与者并且策略为连续的量子博弈做了研究.通过利用一多模光场,该光场是由各个光模之间两两互相纠缠形成的.利用这个方案上述结论可以推广至<span style=\"color:red\">任意</span>多个参与者.并且,随着纠缠度的增加他们的总收益也增加,当每一对双模光场达到最大纠缠时,他们的总收益亦将最大.","authors":[{"authorName":"周杰","id":"987d9c27-25c8-4ab5-a7a7-42ae1789f057","originalAuthorName":"周杰"},{"authorName":"李筠","id":"657bfded-5633-448e-b649-4fd6c0c8138f","originalAuthorName":"李筠"},{"authorName":"马雷","id":"bcaedf3f-1a97-4300-8831-7c1e4ee237cf","originalAuthorName":"马雷"}],"doi":"10.3969/j.issn.1007-5461.2006.02.010","fpage":"173","id":"9f16cef7-1170-400b-abbe-6fa6ed42c568","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":"83f29e7c-abf7-43a1-848a-f5e7decb5ae0","keyword":"量子信息","originalKeyword":"量子信息"},{"id":"c78c2ee9-a879-49c1-af20-d1b1f03dcd76","keyword":"量子博弈","originalKeyword":"量子博弈"},{"id":"67bb4886-1c3a-4d98-bee5-969ed55d4477","keyword":"多人博弈","originalKeyword":"多人博弈"},{"id":"dcae6cbe-1858-4d8d-ae3b-d0c93fd0ebd1","keyword":"量子纠缠","originalKeyword":"量子纠缠"},{"id":"a1bfb925-13ec-4cba-82aa-c9073b05f631","keyword":"连续变量","originalKeyword":"连续变量"}],"language":"zh","publisherId":"lzdzxb200602010","title":"<span style=\"color:red\">任意</span>多入的量子博弈","volume":"23","year":"2006"},{"abstractinfo":"王和闫设计出利用两步方法确定性地实现远程制备单粒子态,受到这个思想的启发,研究了<span style=\"color:red\">任意</span>形式双粒子态的远程制备.在此方案中,两个非最大纠缠GHZ态用作量子通道,制备者Alice将已知态的全部信息分割为两部分,一部分为实系数部分,另一部分为相因子部分.制备者Alice执行两次投影测量并将测量结果用4比特经典信息告诉Bob,远方接收者Bob可以通过合适的幺正变换以概率4|βγ|2成功地获得目标态,此成功概率比刘的方案高,这也是本方案的优点所在,因为在刘的方案中只有二粒子实系数态或赤道态的远程制备才能达到这个概率值.","authors":[{"authorName":"石国芳","id":"cce9374f-bf50-46fd-a6f9-a763b61d30da","originalAuthorName":"石国芳"}],"doi":"10.3969/j.issn.1007-5461.2011.04.005","fpage":"414","id":"6cacc386-8d3f-4c51-a504-3a2fbc340384","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":"8fdf9ec7-5db0-448b-b5b6-9a1cfa51d190","keyword":"量子光学","originalKeyword":"量子光学"},{"id":"16e17573-1f67-4312-ae61-fc72054422e5","keyword":"远程态制备","originalKeyword":"远程态制备"},{"id":"3d765c9d-ac21-4ea2-b643-42a0b5beac66","keyword":"GHZ态","originalKeyword":"GHZ态"}],"language":"zh","publisherId":"lzdzxb201104005","title":"远程制备<span style=\"color:red\">任意</span>双粒子态","volume":"28","year":"2011"},{"abstractinfo":"量子信息传输是量子信息的一个重要分支.以自旋链上单态量子信息的传输为基础,详细讨论了两态和三态信息在自旋链上的传输,并进一步推广至<span style=\"color:red\">任意</span>态的情形.最终得出在自旋链上两态、三态乃至<span style=\"color:red\">任意</span>多态的量子信息传输的概率公式,以及自旋链完备传输<span style=\"color:red\">任意</span>态信息的条件.从而为<span style=\"color:red\">任意</span>多态量子信息的完备传输提供了一套切实可行的理论方案.","authors":[{"authorName":"任恒峰","id":"a9a9649a-1b31-4db4-9d18-a0a58d194262","originalAuthorName":"任恒峰"},{"authorName":"王清亮","id":"f913ac9f-2048-4634-8930-2e05ebff7137","originalAuthorName":"王清亮"},{"authorName":"侯胜侠","id":"e51047b8-de63-4254-8c6d-dbefa83ac52b","originalAuthorName":"侯胜侠"},{"authorName":"连润明","id":"0889f522-0851-4c9a-ae12-8e01bb497b77","originalAuthorName":"连润明"},{"authorName":"杨瑞","id":"176c878a-1422-4969-9c9b-9cb6ce0a910c","originalAuthorName":"杨瑞"}],"doi":"10.3969/j.issn.1007-5461.2012.05.010","fpage":"572","id":"9ab68fd7-eb40-4f6d-92f1-cfc194bf9665","issue":"5","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":"cf1fed39-a1c0-41d4-bf5e-c80aacb5a740","keyword":"量子信息","originalKeyword":"量子信息"},{"id":"4d236764-c1a4-4f08-a5eb-b0603e845785","keyword":"完备传输","originalKeyword":"完备传输"},{"id":"39b9c0d9-0b47-4d4a-9196-4e1a8ecc747f","keyword":"自由演化","originalKeyword":"自由演化"},{"id":"8d55d1f3-0333-49a0-85cc-e28f881d5762","keyword":"自旋链","originalKeyword":"自旋链"}],"language":"zh","publisherId":"lzdzxb201205010","title":"<span style=\"color:red\">任意</span>态量子信息在自旋链上的传输","volume":"29","year":"2012"},{"abstractinfo":"通过把Berreman近似下<span style=\"color:red\">任意</span>形状的表面沟槽用傅里叶级数展开,写成正弦函数和的形式,将Fukuda等人的理论应用于双轴向列相液晶中,考虑表面弹性项的作用后得到了<span style=\"color:red\">任意</span>形状的沟槽对双轴液晶产生的方位锚定能.在一定的近似条件下得到约化锚定能随着沟槽的方向与液晶主指向矢之间的夹角的变化情况,讨论了双轴弹性常数对液晶易<span style=\"color:red\">取向</span>方向的影响.","authors":[{"authorName":"郑桂丽","id":"e5abd968-3b2c-4ccd-bc7a-ce7567296904","originalAuthorName":"郑桂丽"},{"authorName":"李根堂","id":"b8c9232e-4c24-4fae-8e2f-1879a7d5195b","originalAuthorName":"李根堂"},{"authorName":"张志东","id":"88b2faf1-3d4e-464b-a1fb-427c074cd24c","originalAuthorName":"张志东"}],"doi":"10.3788/YJYXS20112602.0137","fpage":"137","id":"ff4610d7-3865-4187-bc9e-4e9cb454e1f4","issue":"2","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示   "},"keywords":[{"id":"68db380f-c9cf-4f8d-aea8-d9b847c5661a","keyword":"双轴向列相液晶","originalKeyword":"双轴向列相液晶"},{"id":"79f1ede3-82da-41b7-a8ed-1906862d3264","keyword":"沟槽","originalKeyword":"沟槽"},{"id":"49ce565a-459e-431c-9392-4bf0dd8fc692","keyword":"傅里叶级数","originalKeyword":"傅里叶级数"},{"id":"66f5b56c-35bc-4f04-a75f-822bb9b26ef9","keyword":"锚定能","originalKeyword":"锚定能"}],"language":"zh","publisherId":"yjyxs201102002","title":"Berreman近似下<span style=\"color:red\">任意</span>形状表面沟槽对双轴向列相方位锚定的影响","volume":"26","year":"2011"},{"abstractinfo":"无衍射光束由于其中心光斑尺寸小、传播中无衍射等特性被广泛关注.提出了一种相位全息图产生<span style=\"color:red\">任意</span>阶次和位置的无衍射光束阵列的方法.设计具有相同特征值的相全息图阵列,即阵列中每幅相全息图在频谱面上产生相同半径的亮环,并把相全息图阵列写入<span style=\"color:red\">空间</span>光调制器,由于傅里叶变换平移不变性,相全息图阵列在频谱面上仍产生唯一能量集中的亮环,通过环形滤波器将其滤出,再次进行傅里叶变换,便得到无衍射光束阵列,并且每个无衍射光束的位置和阶次都可以<span style=\"color:red\">任意</span>设置.理论分析和实验均证明了该方法的可行性.","authors":[{"authorName":"胡名西","id":"5a7a24fa-0c59-42bd-a404-e6f1779000d7","originalAuthorName":"胡名西"},{"authorName":"田劲东","id":"12e5701f-b2f4-4416-b6cc-7416b08bfc58","originalAuthorName":"田劲东"},{"authorName":"王瑞松","id":"d0d1f9c2-1c3c-4b50-9026-d8e368ca964c","originalAuthorName":"王瑞松"},{"authorName":"李东","id":"94c2371d-bb9c-491c-b872-b648157595e3","originalAuthorName":"李东"}],"doi":"10.3969/j.issn.1007-5461.2011.02.006","fpage":"157","id":"bccd73a4-8829-4db3-a7a1-deb2cdd311d2","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":"cba687a5-76ec-4ed2-bab7-215463abc50d","keyword":"信息光学","originalKeyword":"信息光学"},{"id":"13a6b4f1-73d8-4c39-be1a-a1addef5cb3d","keyword":"相位全息图","originalKeyword":"相位全息图"},{"id":"1a2a4e86-3087-41ba-b085-660a13093ccc","keyword":"阵列无衍射光束","originalKeyword":"阵列无衍射光束"},{"id":"dadfdd09-d629-44b7-bf92-c2be8af39462","keyword":"<span style=\"color:red\">空间</span>光调制器","originalKeyword":"空间光调制器"}],"language":"zh","publisherId":"lzdzxb201102006","title":"相全息图产生<span style=\"color:red\">任意</span>阶无衍射光束阵列的理论和实验","volume":"28","year":"2011"},{"abstractinfo":"建立了分析含<span style=\"color:red\">任意</span>形状分层的缝纫增强复合材料层合板压缩屈曲问题的连续分析模型.该模型允许缝纫层合板含有一个或多个形状不同的分层.分析结果表明,缝纫针脚在分层区域的分布、缝纫密度和缝线的等效刚度系数对分层子板的压缩屈曲应变均有较大影响.","authors":[{"authorName":"桂良进","id":"30212611-abf1-4ca4-9439-39e0a26c4371","originalAuthorName":"桂良进"},{"authorName":"郦正能","id":"20704d89-c7b5-4df5-ab09-a5c625e6b6e3","originalAuthorName":"郦正能"},{"authorName":"章怡宁","id":"b78d00c6-b31e-4f26-ad44-77d2424dd93c","originalAuthorName":"章怡宁"},{"authorName":"杨旭","id":"0b09f22f-0869-4fdb-bc06-7ab708e1546a","originalAuthorName":"杨旭"}],"doi":"10.3321/j.issn:1000-3851.2001.02.023","fpage":"97","id":"7c9e1773-8b20-462a-a85a-13f12fe5093d","issue":"2","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":"05dc3094-9596-42fd-a6d6-c1212b0d36f7","keyword":"复合材料","originalKeyword":"复合材料"},{"id":"94525ea5-ad13-465a-8a0b-f627b4d51407","keyword":"缝纫","originalKeyword":"缝纫"},{"id":"5e0ce77b-f14e-49e7-9206-2f0a2c200b36","keyword":"层合板","originalKeyword":"层合板"},{"id":"fb8f2a76-b1f5-4323-9ed2-c6e139d1e36c","keyword":"分层屈曲","originalKeyword":"分层屈曲"}],"language":"zh","publisherId":"fhclxb200102023","title":"含<span style=\"color:red\">任意</span>分层缝纫正交层合板压缩屈曲分析","volume":"18","year":"2001"},{"abstractinfo":"为了提高量子密钥分配的安全性和效率,利用量子纠缠交换的规律,提出了基于纠缠交换的量子密钥分配协议.通信双方通过简单的Bell测量建立起共享密钥,窃听者不可能窃取密钥而不被发现.该协议与其它分配协议的不同在于,可以实现对<span style=\"color:red\">任意</span>两个Bell态进行Bell测量达到量子密钥分配的目的.协议的实现只需要EPR粒子对,而不需要制备多粒子纠缠态.分析结果表明,此协议只用到两粒子的纠缠态,不需要进行幺正操作,它不仅能够保证密钥分配的安全性,而且简单高效.","authors":[{"authorName":"刘林曜","id":"ea7979d3-ba27-41ab-af8a-79b8d4a03aa9","originalAuthorName":"刘林曜"},{"authorName":"胡孟军","id":"bf2a9ebf-8246-40b9-804d-155b35cf6021","originalAuthorName":"胡孟军"},{"authorName":"吕洪君","id":"4259cbf5-b1a6-44ac-9478-61976028bae0","originalAuthorName":"吕洪君"},{"authorName":"解光军","id":"d88530cd-534b-48ff-8230-ce3495d4d04e","originalAuthorName":"解光军"}],"doi":"10.3969/j.issn.1007-5461.2013.04.009","fpage":"439","id":"ed62e4f2-dc78-49d9-920d-058073a14419","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":"7cae8490-ff2e-4cd2-a805-16cd51aac291","keyword":"量子光学","originalKeyword":"量子光学"},{"id":"adaf8519-67e8-456b-883f-2f6faa89eab0","keyword":"量子通信","originalKeyword":"量子通信"},{"id":"05741dd7-6c17-4072-9850-6a79eac798e4","keyword":"量子密钥分配","originalKeyword":"量子密钥分配"},{"id":"ae13ea41-997e-4cac-b181-667c1d97a154","keyword":"量子纠缠交换","originalKeyword":"量子纠缠交换"},{"id":"cc5851bb-c792-4f4b-bd31-1dde167f43eb","keyword":"贝尔测量","originalKeyword":"贝尔测量"}],"language":"zh","publisherId":"lzdzxb201304009","title":"基于<span style=\"color:red\">任意</span>Bell态的量子密钥分配","volume":"30","year":"2013"}],"totalpage":823,"totalrecord":8222}