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","authors":[{"authorName":"李书民","id":"949e304a-c159-49a4-bc4f-f0958c2a8229","originalAuthorName":"李书民"},{"authorName":"陈激","id":"b9bbf7a8-9a25-4401-8d1a-f2279e872d8b","originalAuthorName":"陈激"},{"authorName":"周子舫","id":"7e29625a-3331-4145-ae22-0a2891b1fe19","originalAuthorName":"周子舫"},{"authorName":"张声涛","id":"59c64d78-4b57-4a96-b74c-478a7bee68bf","originalAuthorName":"张声涛"}],"doi":"10.3969/j.issn.1007-4627.2002.02.044","fpage":"242","id":"368af14b-aefd-4e7b-aa31-e0a31a36e5c4","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":"4b615df4-2bde-446c-9a2f-a4f1c60471d7","keyword":"激光场","originalKeyword":"激光场"},{"id":"30898d71-8caa-4239-acb6-1b09c8127ef4","keyword":"电子","originalKeyword":"电子"},{"id":"2eecc700-1f41-497a-b0db-6871879bf6ad","keyword":"氢原子","originalKeyword":"氢原子"},{"id":"6610f5d4-284d-43f3-b19a-cefa7f87ba7c","keyword":"自由-自由跃迁","originalKeyword":"自由-自由跃迁"}],"language":"zh","publisherId":"yzhwlpl200202044","title":"激光辅助的电子对氢原子的自由-自由跃迁","volume":"19","year":"2002"},{"abstractinfo":"在一级玻恩近似下, 研究了在激光辅助的电子偶素-反质子碰撞中的反氢合成. 发现在小角范围内, 平行于电子偶素入射方向极化的激光使反氢生成截面变小. 在中等角度范围, 截面有一定的增加, 特别当偏振方向垂直于入射方向时, 截面增加比较明显. ","authors":[{"authorName":"李书民","id":"e27269e2-bae9-4660-b2b6-8df4d2f1744b","originalAuthorName":"李书民"},{"authorName":"陈激","id":"8ab0ccad-4965-481f-8f06-4c12812cd025","originalAuthorName":"陈激"},{"authorName":"周子舫","id":"5ae54b86-07db-4161-9b7d-add349854298","originalAuthorName":"周子舫"},{"authorName":"张声涛","id":"a7d33062-d527-495c-9af7-44e6ce65a660","originalAuthorName":"张声涛"}],"doi":"10.3969/j.issn.1007-4627.2002.z1.043","fpage":"145","id":"450d5241-3562-4511-9263-e480d079babb","issue":"z1","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":"356f3f5c-749c-4f66-b5b1-570f192f0a7d","keyword":"激光场","originalKeyword":"激光场"},{"id":"5859c64f-aed7-4715-9afd-2c86a58aeafc","keyword":"电子偶素","originalKeyword":"电子偶素"},{"id":"c396e911-adbb-4da4-b629-dce59f4e0511","keyword":"反质子","originalKeyword":"反质子"},{"id":"e4f7fbc5-5b4a-491b-a8b4-b6d30fbc1351","keyword":"反氢原子","originalKeyword":"反氢原子"}],"language":"zh","publisherId":"yzhwlpl2002z1043","title":"激光辅助的电子偶素对反质子的反氢生成反应","volume":"19","year":"2002"},{"abstractinfo":"利用\"表面电流\"模型, 探讨了激光参数在非相对论区条件下激光与固体靶作用产生的高次谐波的若干性质, 也讨论了在非相对论区条件下劳仑兹力项的修正对高次谐波效率的影响. ","authors":[{"authorName":"扬珽均","id":"f868caee-37e1-4cfc-80b2-974e0d4bc73b","originalAuthorName":"扬珽均"},{"authorName":"陈激","id":"03c87f7d-01a2-4b7b-bcdf-2ced77638391","originalAuthorName":"陈激"},{"authorName":"李书民","id":"50c86e99-f8b2-4a33-b4be-c08c597aeb16","originalAuthorName":"李书民"},{"authorName":"张声涛","id":"e10efac2-9e26-4898-9d24-e7f680359751","originalAuthorName":"张声涛"}],"doi":"10.3969/j.issn.1007-4627.2002.z1.026","fpage":"85","id":"c8c6ee70-1f4e-450d-bf0c-94c0459c5022","issue":"z1","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":"a8fa08ca-ebc0-469c-8f92-4e2d8e3b0737","keyword":"短脉冲激光","originalKeyword":"短脉冲激光"},{"id":"458b10e4-4b04-4646-88eb-a549f6332834","keyword":"高次谐波","originalKeyword":"高次谐波"},{"id":"acbad1a6-2543-4307-a1bb-ba1df9237c8e","keyword":"\"表面电流\"模型","originalKeyword":"\"表面电流\"模型"}],"language":"zh","publisherId":"yzhwlpl2002z1026","title":"短脉冲强激光与固体靶作用在非相对论激光参数区的高次谐波","volume":"19","year":"2002"},{"abstractinfo":"在软光子近似下, 计算了激光场中正电子对反质子的辐射复合过程. 辐射场作为经典场处理, 入射正电子态用Coulomb-Volkov波函数描述, 末道形成的反氢缀饰态由含时间微扰论给出. 理论结果显示激光背景明显削弱了反氢生成截面.","authors":[{"authorName":"李书民","id":"e8421d36-3137-4c15-b85f-67dc17465343","originalAuthorName":"李书民"},{"authorName":"陈激","id":"94f90e29-ed32-42c6-808e-35d07f60bfb8","originalAuthorName":"陈激"},{"authorName":"周子舫","id":"d715b6c6-4a2e-4a2f-a050-5fe9fbafc4e9","originalAuthorName":"周子舫"},{"authorName":"张声涛","id":"fc3bb7ce-d2e0-4b2d-8120-0d22f32c7b25","originalAuthorName":"张声涛"}],"doi":"10.3969/j.issn.1007-4627.2002.z1.044","fpage":"148","id":"22cc2fbe-8760-43b9-84a3-4921d3bff61b","issue":"z1","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":"04110379-4a7b-4209-9d13-5f12a0e0dcdd","keyword":"激光场","originalKeyword":"激光场"},{"id":"03c7a96a-ea0f-4ed4-95dc-0561aecf9400","keyword":"正电子","originalKeyword":"正电子"},{"id":"79140480-ff7d-470a-93d1-ba3b05995e40","keyword":"反质子","originalKeyword":"反质子"},{"id":"20fd3dbe-8576-49c1-93e3-91333e3db321","keyword":"反氢原子","originalKeyword":"反氢原子"}],"language":"zh","publisherId":"yzhwlpl2002z1044","title":"激光场中正电子对反质子的辐射复合反应","volume":"19","year":"2002"},{"abstractinfo":"在质心参考系中研究了激光场中1 MeV质子对基态氢原子的碰撞电离过程. 靶原子的缀饰波函数由含时间微扰论给出, 末道出射电子态用双中心Coulomb-Volkov波函数描述. 计算表明辐射场使出射电子的双重微分截面变小. 敲出电子的能量越高, 截面减小越明显, 但截面中CTC峰的位置基本不受辐射场的影响. ","authors":[{"authorName":"李书民","id":"ece32eb9-fdec-4b45-8d0e-165b98ef5cb9","originalAuthorName":"李书民"},{"authorName":"陈激","id":"63dad91f-58bc-4016-8199-0ba332850c69","originalAuthorName":"陈激"},{"authorName":"周子舫","id":"395b23c9-c984-45d8-bbfd-32a67621b166","originalAuthorName":"周子舫"},{"authorName":"张声涛","id":"2e7d1341-b5e3-4b2f-b8cf-7caae3e82319","originalAuthorName":"张声涛"}],"doi":"10.3969/j.issn.1007-4627.2002.z1.045","fpage":"151","id":"c3ea8259-66b2-4519-a4c7-9374303a421c","issue":"z1","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":"ba9cec43-b8a5-4679-bb86-8ea9c0a4400d","keyword":"激光场","originalKeyword":"激光场"},{"id":"216700a1-6a36-4cb1-b0fc-49ec80dce523","keyword":"快质子","originalKeyword":"快质子"},{"id":"c5d47a36-1514-4d46-97d2-3974dceec4a7","keyword":"氢原子","originalKeyword":"氢原子"},{"id":"94c7024e-4a8f-4aea-a28e-a6651bca0ea0","keyword":"碰撞电离","originalKeyword":"碰撞电离"}],"language":"zh","publisherId":"yzhwlpl2002z1045","title":"激光辅助的快质子对氢原子的碰撞电离","volume":"19","year":"2002"},{"abstractinfo":"本文提出一个简单的理论模型,模型认为在超强、超短脉冲P极化激光与固体靶相互作用过程中高次谐波的产生是固体靶表面趋肤层中的相对论电子运动形成的横向和纵向电流发出辐射的非线性叠加的结果.在此模型基础上,得到了高次谐波的角分布,并讨论了谐波转换效率与谐波次数的关系.结果表明,有超过50次的谐波的转换效率在10-6以上.","authors":[{"authorName":"武帅","id":"eb6ae4cc-c7e9-4a00-a6fd-7977fbcfbfc2","originalAuthorName":"武帅"},{"authorName":"詹如娟","id":"2d620fab-f208-445d-8c2f-8b8db6f60b3b","originalAuthorName":"詹如娟"},{"authorName":"陈激","id":"bcf83c2e-a9c1-414b-b654-81a72e6dcf96","originalAuthorName":"陈激"}],"doi":"10.3969/j.issn.1007-5461.2001.04.015","fpage":"352","id":"8ec8624e-d6a9-4e60-bac0-3f073af79583","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":"f2216dfc-352e-49b6-b1fc-9b3ba4407ab9","keyword":"超强、超短脉冲激光","originalKeyword":"超强、超短脉冲激光"},{"id":"0d0dfd71-bd7c-4e06-86c5-97837058b112","keyword":"固体靶","originalKeyword":"固体靶"},{"id":"0d50ed57-e60b-4252-b1f0-8b1a7d009c97","keyword":"等离子体","originalKeyword":"等离子体"},{"id":"7616116d-29a3-4af0-a95c-96239ff67350","keyword":"高次谐波","originalKeyword":"高次谐波"}],"language":"zh","publisherId":"lzdzxb200104015","title":"短脉冲强激光与固体靶作用激发的高次谐波","volume":"18","year":"2001"},{"abstractinfo":"研究了双色共振激光场中电子原子碰撞的自由-自由跃迁过程. 利用三能级模型和旋转波近似得到了靶原子的波函数, 在波恩近似的基础上进一步导出了多道碰撞的微分截面公式. 利用此公式计算了共振激光场中的激发碰撞对整个的碰撞贡献. ","authors":[{"authorName":"张声涛","id":"34ea56d8-6673-4b45-be1f-67f0a9d95020","originalAuthorName":"张声涛"},{"authorName":"陈激","id":"193bc018-fe5c-4351-9cc3-c7ca75cc95c3","originalAuthorName":"陈激"},{"authorName":"李书民","id":"b3b48b5e-1456-409e-9a99-227095f4f97a","originalAuthorName":"李书民"}],"doi":"10.3969/j.issn.1007-4627.2002.z1.024","fpage":"77","id":"326f9bba-05dc-497a-9346-8dffd1662bbc","issue":"z1","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":"2b11f7d2-6f1f-487b-958c-ef1cbb4e42ba","keyword":"共振","originalKeyword":"共振"},{"id":"36f1e519-da24-418c-865f-65794c916eba","keyword":"双色激光场","originalKeyword":"双色激光场"},{"id":"6a3f6f12-fb8e-435e-9c38-a74615b6d940","keyword":"自由-自由跃迁","originalKeyword":"自由-自由跃迁"}],"language":"zh","publisherId":"yzhwlpl2002z1024","title":"在双色共振激光场中电子原子碰撞的自由-自由跃迁过程","volume":"19","year":"2002"},{"abstractinfo":"以能量为1.5 MeV/u,剂量分别为500,750,1000,1250,1500 Gy的电子束对1,2,4,6,8年等5种年份浓香型白酒进行辐照处理;扫描各酒样200~400 nm波段的紫外光谱,根据紫外光谱图的差异,计算了280~300 nm波段的光谱曲线相似度,分析光谱曲线变化规律。结果表明,对于前4种白酒,对照样与辐照样光谱曲线相似度值越小,催陈效果越好;白酒存放时间越久,酒体风格转向老熟所需剂量越小,越容易达到最佳催陈效果;对于8年白酒,辐照剂量超过750 Gy后,白酒体系动态平衡被打破,各单体物质增加,出现返生现象。因此,电子束辐照技术对低年份浓香型白酒催陈效果显著,是一种先进、高效的催陈方法。","authors":[{"authorName":"张苗苗","id":"16f2bee9-e276-4f55-95b1-9e627a4ac276","originalAuthorName":"张苗苗"},{"authorName":"陆栋","id":"6bd2c6ff-fa0f-4deb-9553-bfa0e40d3ab7","originalAuthorName":"陆栋"},{"authorName":"曹国珍","id":"ad44f083-8f23-4d8d-a41c-b6321e181155","originalAuthorName":"曹国珍"},{"authorName":"刘敬","id":"980de600-54b3-4c10-b2b1-7d36c88bd704","originalAuthorName":"刘敬"},{"authorName":"金文杰","id":"9d97782b-4400-438f-aa1a-efaa2ae74455","originalAuthorName":"金文杰"},{"authorName":"王菊芳","id":"7a171c96-4419-441c-8118-cabb35cc1b2c","originalAuthorName":"王菊芳"},{"authorName":"李文建","id":"db0225a5-b939-440c-a47d-2daa37f339b7","originalAuthorName":"李文建"}],"doi":"10.11804/NuclPhysRev.31.02.218","fpage":"218","id":"be399f10-d5ab-444a-9853-693337e4845a","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":"d27824cd-9a7d-40d6-ade5-08e57f3651e9","keyword":"白酒","originalKeyword":"白酒"},{"id":"a87d8a5f-52c5-438d-9818-ac05aa030ecd","keyword":"电子束","originalKeyword":"电子束"},{"id":"59b3d998-0774-4358-b00a-6ad942d1d4f2","keyword":"紫外可见光谱","originalKeyword":"紫外可见光谱"},{"id":"7662c117-7566-4173-b784-d5cf69060062","keyword":"光谱曲线相似度","originalKeyword":"光谱曲线相似度"},{"id":"ef90b8b5-c334-453a-8346-0f1341f1e34b","keyword":"催陈效果","originalKeyword":"催陈效果"}],"language":"zh","publisherId":"yzhwlpl201402017","title":"电子束辐照浓香型白酒催陈效果的研究","volume":"","year":"2014"},{"abstractinfo":"本文对自激脉冲射流喷嘴进行试验设计和数据分析,以自激频率、振幅以及打击力等作为响应函数,研究喷嘴结构与工作压力的配套关系.通过对自激频率和振幅的分析,揭示自激振荡腔内部周期性空化现象及其对自激脉冲形成的影响,从而从解释自激脉冲射流发生机理.根据试验数据,拟合打击力随参数变化的经验公式.最终得出工业应用中典型尺寸范围的自激脉冲喷嘴与自激频率及打击力的关系,为工业设计中的频域调制理论提供了试验数据.","authors":[{"authorName":"王健","id":"265fe8b4-922b-45e5-9565-e4503489274d","originalAuthorName":"王健"},{"authorName":"李江云","id":"e5803cdb-1183-483f-9e58-2ac7da35a182","originalAuthorName":"李江云"},{"authorName":"关凯","id":"9cee6657-deab-42a7-a50c-c230aa9469be","originalAuthorName":"关凯"}],"doi":"","fpage":"678","id":"53bcb726-7c09-4732-9ab6-6788150087b6","issue":"4","journal":{"abbrevTitle":"GCRWLXB","coverImgSrc":"journal/img/cover/GCRWLXB.jpg","id":"32","issnPpub":"0253-231X","publisherId":"GCRWLXB","title":"工程热物理学报 "},"keywords":[{"id":"c1a475aa-4a11-4156-997e-cedfb69c07d2","keyword":"自激","originalKeyword":"自激"},{"id":"a165b8af-f097-4958-8f69-467488fece0b","keyword":"打击力","originalKeyword":"打击力"},{"id":"1372aebb-6885-4e25-9743-c323c04a8163","keyword":"试验设计","originalKeyword":"试验设计"},{"id":"e92b4ac8-987a-4b81-aea6-def655a7d720","keyword":"频率调制","originalKeyword":"频率调制"}],"language":"zh","publisherId":"gcrwlxb201404013","title":"自激脉冲喷嘴装置试验研究","volume":"35","year":"2014"}],"totalpage":35,"totalrecord":343}