{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"Silberberg等利用三芯耦合光波导的暗态现象,实验研究了非线性对相干布居<span style=\"color:red\">囚禁</span>量子效应的影响.然而,对该三芯耦合波导中的非线性传输特征数值计算的研究表明,相干布居<span style=\"color:red\">囚禁</span>与光波导的非线性<span style=\"color:red\">自</span><span style=\"color:red\">囚禁</span>两种效应都可以导致波导中暗态的产生,当两种效应同时作用时,则导致暗态现象的破坏.因此,仅从暗态的变化研究非线性对相干布居<span style=\"color:red\">囚禁</span>的影响是不完备的.在相干布居<span style=\"color:red\">囚禁</span>的理想条件下,非线性影响暗态的阈值功率趋于无穷大,这意味着理想相干布居<span style=\"color:red\">囚禁</span>量子效应不受限于系统的非线性效应.","authors":[{"authorName":"倪程鹏","id":"3799537d-d8bf-4aa3-a32f-e246dfa26431","originalAuthorName":"倪程鹏"},{"authorName":"周桥梁","id":"b4e8f9a4-a990-4b49-a680-d2f80ed50517","originalAuthorName":"周桥梁"},{"authorName":"王文峰","id":"7ba5172b-ae81-4508-a5ca-1d9b1ef5bb7f","originalAuthorName":"王文峰"}],"doi":"10.3969/j.issn.1007-5461.2014.02.012","fpage":"202","id":"3e29545f-826f-41f4-bac8-d0a0bdbc02d2","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":"91ee5f0c-eed0-45e6-a859-c3064bd8e9fa","keyword":"非线性光学","originalKeyword":"非线性光学"},{"id":"32c9b99e-1e34-470c-a575-bd4311cd79da","keyword":"暗态","originalKeyword":"暗态"},{"id":"d99bd745-291d-4141-a972-872bcaced259","keyword":"数值模拟","originalKeyword":"数值模拟"},{"id":"991833c9-a06a-496a-8b2a-e0b8972bf46f","keyword":"三芯耦合波导","originalKeyword":"三芯耦合波导"},{"id":"5ba0996e-deb2-4576-9cd6-e8a1016ba580","keyword":"相干布居<span style=\"color:red\">囚禁</span>","originalKeyword":"相干布居囚禁"},{"id":"b20930b5-50de-45d1-92a8-739e11e5a479","keyword":"<span style=\"color:red\">自</span><span style=\"color:red\">囚禁</span>","originalKeyword":"自囚禁"}],"language":"zh","publisherId":"lzdzxb201402012","title":"三芯耦合波导中暗态的研究","volume":"31","year":"2014"},{"abstractinfo":"提出了一个利用热<span style=\"color:red\">囚禁</span>离子来实现两人量子囚徒困境的方案.用双色激光同时照射两个离子,振荡模处于虚激发状态,所以系统对热场不敏感.此外,由于量子博弈中基本的逻辑门可以直接构造,方案相对简单.","authors":[{"authorName":"谢鸿","id":"5438508b-f3e4-415a-b0fa-476501dd0cfe","originalAuthorName":"谢鸿"},{"authorName":"李洪才","id":"5e6a857b-301d-4176-b34f-3ce81315dbc2","originalAuthorName":"李洪才"},{"authorName":"杨熔灿","id":"1b71b1b3-9b7f-4fb9-959b-147060099843","originalAuthorName":"杨熔灿"},{"authorName":"林秀","id":"0aed1ebf-83e3-42d8-b30c-10d69f1b43c0","originalAuthorName":"林秀"},{"authorName":"黄志平","id":"86fd9290-a25d-4fdc-b0c3-e7e30ef1b24a","originalAuthorName":"黄志平"}],"doi":"10.3969/j.issn.1007-5461.2008.06.009","fpage":"698","id":"8ccec085-60f7-44b7-b469-862f66507549","issue":"6","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":"74480445-3b29-4959-9b48-cd4e8fa4240a","keyword":"量子光学","originalKeyword":"量子光学"},{"id":"906ff68d-beff-40cb-a890-aa24cb7ed0fd","keyword":"量子囚徒困境","originalKeyword":"量子囚徒困境"},{"id":"7b1c17d0-11ba-4ab0-a6be-d0fb23a1c205","keyword":"<span style=\"color:red\">囚禁</span>离子","originalKeyword":"囚禁离子"},{"id":"02e44871-d4c0-4a2d-8883-7026d7fd3a71","keyword":"最大纠缠","originalKeyword":"最大纠缠"}],"language":"zh","publisherId":"lzdzxb200806009","title":"利用<span style=\"color:red\">囚禁</span>离子实现量子博弈","volume":"25","year":"2008"},{"abstractinfo":"本文就近二十年来国际上用于三维限制中性原子运动的磁<span style=\"color:red\">囚禁</span>原理、方案、特点及其最新发展进行了系统介绍与综述.根据构成磁阱的装置大小、磁场特征以及产生磁场方式的不同,可以将<span style=\"color:red\">囚禁</span>原子的各种磁阱分为宏观静磁<span style=\"color:red\">囚禁</span>、微观静磁<span style=\"color:red\">囚禁</span>和微波或交流磁<span style=\"color:red\">囚禁</span>三大类.最后,文章简单介绍了中性原子磁<span style=\"color:red\">囚禁</span>技术在玻色-爱因斯坦凝聚(BEC)和原子芯片中的最新应用.","authors":[{"authorName":"胡建军","id":"b52b5384-5756-48fb-a697-c237050dbbcd","originalAuthorName":"胡建军"},{"authorName":"印建平","id":"0839734e-cec1-4efe-a278-f28471c510e6","originalAuthorName":"印建平"}],"doi":"10.3969/j.issn.1007-5461.2003.03.001","fpage":"257","id":"7892ad35-f714-44f6-b32c-f6dc77bbf8f1","issue":"3","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":"08ed73ae-f3ff-4eac-afb1-ce5f6d3bb1ec","keyword":"中性原子","originalKeyword":"中性原子"},{"id":"afcd8197-0581-43cd-82c2-d51ac124d264","keyword":"磁<span style=\"color:red\">囚禁</span>技术","originalKeyword":"磁囚禁技术"},{"id":"f2b247b1-3566-461f-afea-c52a8d94245e","keyword":"玻色-爱因斯坦凝聚","originalKeyword":"玻色-爱因斯坦凝聚"},{"id":"2547b709-d8aa-4b18-968b-e4b3a78c6a22","keyword":"原子芯片","originalKeyword":"原子芯片"}],"language":"zh","publisherId":"lzdzxb200303001","title":"中性原子的磁<span style=\"color:red\">囚禁</span>技术及其最新发展与应用","volume":"20","year":"2003"},{"abstractinfo":"<span style=\"color:red\">囚禁</span>汞离子的光微波双共振实验是开展汞离子微波频标的实验基础.二级Zeeman效应是影响频率稳定度和磁场效应的重要因素之一.利用光学微波双共振方法测量了<span style=\"color:red\">囚禁</span>199Hg+离子基态Zeeman分裂.通过减小微波扫描的频率范围,得到钟跃迁频率和谱线线宽.采用磁屏蔽材料(坡莫合金)对离子阱<span style=\"color:red\">囚禁</span>区域的磁场进行屏蔽.使得<span style=\"color:red\">囚禁</span>汞离子的钟跃迁谱线的线宽减小到1.5 Hz.相对于无磁场屏蔽时,钟跃迁频率减小13.5 Hz,并利用二级Zeeman效应估算出磁屏蔽后离子<span style=\"color:red\">囚禁</span>区域磁场大小为0.1高斯.","authors":[{"authorName":"黄雄","id":"debe7788-8e40-4e60-8878-3154728681cd","originalAuthorName":"黄雄"},{"authorName":"杨玉娜","id":"0674e661-dcdc-4eab-b9ec-e90ea49d9954","originalAuthorName":"杨玉娜"},{"authorName":"柳浩","id":"72f007df-9d80-4b81-8e57-21261614997a","originalAuthorName":"柳浩"},{"authorName":"高克林","id":"5057711f-96da-442f-8269-20ccf2724b85","originalAuthorName":"高克林"},{"authorName":"佘磊","id":"98d88501-a5b3-4dcb-95ef-6270e782c440","originalAuthorName":"佘磊"},{"authorName":"李交美","id":"667b222a-6667-4f4f-b2a5-f05c529f75fc","originalAuthorName":"李交美"}],"doi":"10.3969/j.issn.1007-5461.2011.01.004","fpage":"19","id":"d9ea5d41-91de-42ca-828d-960cfdeda855","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":"dd5ffd06-1927-4f1f-bb59-83687073ee44","keyword":"光谱学","originalKeyword":"光谱学"},{"id":"8878864a-ff35-4a77-aa09-336e0f0a36cb","keyword":"<span style=\"color:red\">囚禁</span>汞离子","originalKeyword":"囚禁汞离子"},{"id":"c7b799a5-8c6c-4420-a7e3-a8647d178305","keyword":"磁场效应","originalKeyword":"磁场效应"},{"id":"858ca818-c2f2-4888-bcad-38f1aa0822ad","keyword":"线宽","originalKeyword":"线宽"}],"language":"zh","publisherId":"lzdzxb201101004","title":"<span style=\"color:red\">囚禁</span>汞(199Hg+)离子Zeeman谱及磁场效应","volume":"28","year":"2011"},{"abstractinfo":"基于以前的研究结果,采用函数级数展开法,研究了Paul阱中在非理想射频<span style=\"color:red\">囚禁</span>场作用下、考虑二次谐波φ=U-V1cosΩt-Vscos 2Ωt时<span style=\"color:red\">囚禁</span>离子运动特性,得到了单个<span style=\"color:red\">囚禁</span>离子运动Mathieu方程的解析解和z方向离子运动的特征频率(宏运动,微运动)随倍频参数的变化规律.","authors":[{"authorName":"陈图淼","id":"58df5a5f-abb5-47b1-8692-b39725eaebfa","originalAuthorName":"陈图淼"},{"authorName":"聂宗秀","id":"171f9907-05c2-4a1d-ae76-bc4e9d860fb9","originalAuthorName":"聂宗秀"}],"doi":"10.3969/j.issn.1007-5461.2003.01.010","fpage":"51","id":"ed1bab6e-c860-4363-bdea-96aa022b5df3","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":"476b6d5e-face-414c-8057-5ac02ed8a9ff","keyword":"运动特性","originalKeyword":"运动特性"},{"id":"11d82e05-6a55-4cd2-a0e5-90c70f66b7c1","keyword":"倍频效应","originalKeyword":"倍频效应"},{"id":"393c4d15-fe79-420c-a3bc-01a2023a8b55","keyword":"Paul阱","originalKeyword":"Paul阱"}],"language":"zh","publisherId":"lzdzxb200301010","title":"Paul阱中射频源倍频作用下<span style=\"color:red\">囚禁</span>离子运动特性","volume":"20","year":"2003"},{"abstractinfo":"通过非线性变换和特殊设计结点的B样条函数研究计算了<span style=\"color:red\">囚禁</span>于巴基球内的氢原子里德堡能级结构和振子强度. 结果表明, 巴基球等效势阱深度可以有选择的影响和改变里德堡原子的特性; <span style=\"color:red\">囚禁</span>原子拥有很多自由原子所没有的奇特性质. ","authors":[{"authorName":"张现周","id":"09c4cf95-a682-4549-903b-20409b69ee63","originalAuthorName":"张现周"},{"authorName":"焦照勇","id":"4eee1b4a-5ea3-4de1-a609-c37a010c5edd","originalAuthorName":"焦照勇"},{"authorName":"饶建国","id":"5e3fa3f0-7a8b-4b4c-9e72-048fe3703221","originalAuthorName":"饶建国"}],"doi":"10.3969/j.issn.1007-4627.2002.02.047","fpage":"253","id":"99a0b71a-5dc1-4962-a09f-ffc27bdd7f0f","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":"13a4be3a-8168-46ee-a390-7e9c302926b8","keyword":"巴基球","originalKeyword":"巴基球"},{"id":"5de53973-06cf-4c45-9864-36b69c971521","keyword":"里德堡原子","originalKeyword":"里德堡原子"},{"id":"00810709-6afd-40e0-9ad3-62e8105d549d","keyword":"非线性变换","originalKeyword":"非线性变换"},{"id":"c131c591-c00c-412b-9b76-c19ed339c8c0","keyword":"B 样条函数方法","originalKeyword":"B 样条函数方法"}],"language":"zh","publisherId":"yzhwlpl200202047","title":"<span style=\"color:red\">囚禁</span>于巴基球内的原子的里德堡特性","volume":"19","year":"2002"},{"abstractinfo":"<span style=\"color:red\">囚禁</span>离子的纠缠态在量子计算和量子信息方面有极为重要的应用.由于量子系统的特性,激光强度不可避免地发生涨落,其对<span style=\"color:red\">囚禁</span>离子的纠缠度有显著影响.从反J-C模型出发,利用共生纠缠度标准,分析了激光强度涨落对系统纠缠动力学的影响,并与利用J-C模型时的情形做了适当对比.结果显示:激光强度涨落产生的噪声使两离子纠缠度随时间呈现类似指数衰减；激光强度较弱时,利用正反J-C模型所得系统纠缠动力学有显著差别.","authors":[{"authorName":"范朝阳","id":"89e82dc0-f1e6-4e87-a04d-b25ce386529d","originalAuthorName":"范朝阳"},{"authorName":"王中结","id":"3e12a288-1ef0-47a3-92cb-0ff736d04fc7","originalAuthorName":"王中结"}],"doi":"10.3969/j.issn.1007-5461.2011.05.011","fpage":"577","id":"3f4cf6a9-883d-4932-8d40-bbc191af5f40","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":"bfac5db0-6c99-485b-8670-da5fbbf7e5b3","keyword":"量子光学","originalKeyword":"量子光学"},{"id":"f13aa30a-f712-4297-9dc4-0f77c87a58f9","keyword":"强度涨落","originalKeyword":"强度涨落"},{"id":"7099bd8b-c63c-483d-a3e9-d1881458688b","keyword":"平均光子数","originalKeyword":"平均光子数"},{"id":"df6cf9c9-d920-4a98-a94f-387c99b562bb","keyword":"纠缠动力学","originalKeyword":"纠缠动力学"},{"id":"453bea64-4fd5-47ca-b79b-3e634c5c74ad","keyword":"共生纠缠度","originalKeyword":"共生纠缠度"}],"language":"zh","publisherId":"lzdzxb201105011","title":"激光强度涨落对两<span style=\"color:red\">囚禁</span>离子纠缠度的影响","volume":"28","year":"2011"},{"abstractinfo":"运用全量子理论的方法,研究了在驻波激光场中单个<span style=\"color:red\">囚禁</span>离子布居数反转的动力学特性,分别讨论非线性参数η和驻波场的相位φ对离子布居数反转崩塌-复原现象的影响.结果表明,随着η的增大,离子的布居数反转崩塌-复原的周期变短,振荡频率变大.但当η超过某一临界值时,离子布居数反转崩塌-复原的轮廓变得不明显,另外,驻波激光场的相位也对<span style=\"color:red\">囚禁</span>离子布居数反转的动力学特性有明显的影响,随着φ的增大,离子的布居数反转崩塌-复原的周期变大,振荡频率变大.","authors":[{"authorName":"李剑","id":"86172acf-6f8e-416d-994d-f167081ff883","originalAuthorName":"李剑"}],"doi":"10.3969/j.issn.1007-5461.2013.04.013","fpage":"461","id":"b17efe90-e779-4a07-9154-9c7d97f6fc83","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":"0c7faf69-168c-424c-9b13-37ff97a3da25","keyword":"量子光学","originalKeyword":"量子光学"},{"id":"e7e81996-ab51-4581-815b-629153a18e19","keyword":"布居数反转","originalKeyword":"布居数反转"},{"id":"02c560d1-9591-4ca5-afbb-a082ad70a5df","keyword":"全量子理论","originalKeyword":"全量子理论"},{"id":"a7e62925-8dc6-4a61-b52b-09abbb2bb36c","keyword":"非线性相干态","originalKeyword":"非线性相干态"}],"language":"zh","publisherId":"lzdzxb201304013","title":"非线性<span style=\"color:red\">囚禁</span>离子模型中布居数反转演化","volume":"30","year":"2013"},{"abstractinfo":"用饱和吸收光谱法对二极管激光器进行了稳频，使得激光 器的等效线宽小于1～MHz，并利用声光调制器使激光的频移量得到 控制，能满足激光冷却与<span style=\"color:red\">囚禁</span>原子对激光频率稳定性和频移量的要 求，实现了Rb原子的激光<span style=\"color:red\">囚禁</span>。","authors":[{"authorName":"Wang Jin","id":"a2c88aa8-14b7-4cbc-93c6-13e6797368da","originalAuthorName":"Wang Jin"},{"authorName":"王谨","id":"3ddc0cc3-c703-4cf5-85ba-cde7d4e8a5b3","originalAuthorName":"王谨"},{"authorName":"柳晓军","id":"1df7a40c-7235-4e37-a51f-d15e3a05a9b8","originalAuthorName":"柳晓军"},{"authorName":"李交美","id":"4dc54f44-ffdc-4e1c-8532-294fc19c277f","originalAuthorName":"李交美"},{"authorName":"江开军","id":"d210cb88-130c-4dcd-a479-baafcd827475","originalAuthorName":"江开军"},{"authorName":"詹明生","id":"6a5978e7-ecf4-4e1b-926f-cca3ebbb87c4","originalAuthorName":"詹明生"}],"doi":"10.3969/j.issn.1007-5461.2000.01.009","fpage":"43","id":"9deeb55f-3c1c-40fe-a2f7-24816fe59469","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":"a20a35ef-2838-436b-b854-25f69610610d","keyword":"饱和吸收光谱","originalKeyword":"饱和吸收光谱"},{"id":"94badc07-65ea-49c5-a27e-feaddd119665","keyword":"二极管激光器稳频","originalKeyword":"二极管激光器稳频"},{"id":"6cc316ae-dc67-4987-acdd-a809e4ab51fa","keyword":"激光<span style=\"color:red\">囚禁</span>原子","originalKeyword":"激光囚禁原子"}],"language":"zh","publisherId":"lzdzxb200001009","title":"用于激光原子<span style=\"color:red\">囚禁</span>的二极管激光器的稳频和移频","volume":"17","year":"2000"},{"abstractinfo":"在Thomas-Fermi半经典近似适用条件下,求得了理想费米气体在n维广义幂律势阱中的态密度,进而研究了粒子数密度的空间分布,内能,热容量的空间变化以及等效化学势的一级近似.定义了绝对零度下的特征长度,求出了理想费米气体在n维广义幂律势阱中的有效<span style=\"color:red\">囚禁</span>范围.利用两个例子,揭示了理想费米气体的有效<span style=\"color:red\">囚禁</span>范围与外势形式,粒子数,粒子质量以及势场圆频率的依赖关系.","authors":[{"authorName":"袁都奇","id":"a55ac3eb-db04-4282-b091-2d033f04ef2d","originalAuthorName":"袁都奇"},{"authorName":"王参军","id":"b3a8f0b2-bf77-4f26-920b-712ca96302c9","originalAuthorName":"王参军"}],"doi":"","fpage":"425","id":"28d6e664-25fa-4633-ab15-1abb75f9bf8d","issue":"6","journal":{"abbrevTitle":"DWWLXB","coverImgSrc":"journal/img/cover/DWWLXB.jpg","id":"19","issnPpub":"1000-3258","publisherId":"DWWLXB","title":"低温物理学报   "},"keywords":[{"id":"93fed190-8c41-484a-a54a-bd65a90c85ae","keyword":"理想费米气体","originalKeyword":"理想费米气体"},{"id":"5e5678c0-b7fb-47d9-b66c-cb5d2f71d313","keyword":"有效<span style=\"color:red\">囚禁</span>范围","originalKeyword":"有效囚禁范围"},{"id":"28e961ea-385b-4cb3-b23b-a04c42eb596c","keyword":"空间分布","originalKeyword":"空间分布"},{"id":"e182936e-97cc-4b12-8f30-2e1ff7222541","keyword":"n维势阱","originalKeyword":"n维势阱"}],"language":"zh","publisherId":"dwwlxb201406004","title":"理想费米气体在n维势阱中的空间分布与有效<span style=\"color:red\">囚禁</span>范围","volume":"36","year":"2014"}],"totalpage":405,"totalrecord":4041}